File: analyses.tex

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\section{LEP and SLC analyses}\typeout{Handling analysis ALEPH_1991_S2435284}\subsection[ALEPH\_1991\_S2435284]{ALEPH\_1991\_S2435284\,\cite{Decamp:1991uz}}
\textbf{Hadronic Z decay charged multiplicity measurement}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} ALEPH (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2435284}{2435284}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Lett. B, 273, 181 (1991)
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent The charged particle multiplicity distribution of hadronic Z decays, as measured on the peak of the Z resonance using the ALEPH detector at LEP. The unfolding procedure was model independent, and the distribution was found to have a mean of $20.85 \pm 0.24$, Comparison with lower energy data supports the KNO scaling hypothesis. The shape of the multiplicity distribution is well described by a log-normal distribution, as predicted from a cascading model for multi-particle production.

\clearpage


\clearpage

\typeout{Handling analysis ALEPH_1996_S3196992}\subsection[ALEPH\_1996\_S3196992]{ALEPH\_1996\_S3196992\,\cite{Buskulic:1995au}}
\textbf{Measurement of the quark to photon fragmentation function}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} ALEPH (LEP Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3196992}{3196992}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys.C69:365-378,1996
  \item DOI: \href{http://dx.doi.org/10.1007/s002880050037}{10.1007/s002880050037}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+e^-\to$ jets with $\pi$ and $\eta$ decays turned off.\end{itemize}

\noindent Earlier measurements at LEP of isolated hard photons in hadronic Z decays, attributed to radiation from primary quark pairs, have been extended in the ALEPH experiment to include hard photon production inside hadron jets. Events are selected where all particles combine democratically to form hadron jets, one of which contains a photon with a fractional energy $z > 0.7$. After statistical subtraction of non-prompt photons, the quark-to-photon fragmentation function, $D(z)$, is extracted directly from the measured 2-jet rate.

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\clearpage

\typeout{Handling analysis ALEPH_1996_S3486095}\subsection[ALEPH\_1996\_S3486095]{ALEPH\_1996\_S3486095\,\cite{Barate:1996fi}}
\textbf{Studies of QCD with the ALEPH detector.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} ALEPH (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3486095}{3486095}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rept., 294, 1--165 (1998)
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Summary paper of QCD results as measured by ALEPH at LEP 1. The publication includes various event shape variables, multiplicities (identified particles and inclusive), and particle spectra.

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\clearpage

\typeout{Handling analysis ALEPH_1999_S4193598}\subsection[ALEPH\_1999\_S4193598]{ALEPH\_1999\_S4193598\,\cite{Barate:1999bg}}
\textbf{Scaled energy distribution of $D^*$ at LEP}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} ALEPH (LEP)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4193598}{4193598}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:hschulz@physik.hu-berlin.de}{hschulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C16:597-611,2000
  \item hep-ex/9909032
  \item CERN-EP-99-094
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic $Z$ decays at 91.2~GeV.\end{itemize}

\noindent Study of Charm Production in $Z$ Decays. Here, only the scaled energy distribution of $D^{*\pm}$ is implemented. Should be very important for fragmentation tuning.

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\typeout{Handling analysis ALEPH_2001_S4656318}\subsection[ALEPH\_2001\_S4656318]{ALEPH\_2001\_S4656318\,\cite{Heister:2001jg}}
\textbf{Study of the fragmentation of b quarks into B mesons at the Z peak}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} ALEPH (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4656318}{4656318}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B512:30-48,2001.
  \item hep-ex/0106051
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurement of the $b$-quark fragmentation function by ALEPH using LEP 1 data. The fragmentation function for both weakly decaying and leading $b$-quarks has been determined. The data used for the plots has been renormalised to give a differential distribution rather than the bin-by-bin average in HEPDATA.

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\typeout{Handling analysis ALEPH_2002_S4823664}\subsection[ALEPH\_2002\_S4823664]{ALEPH\_2002\_S4823664\,\cite{Heister:2001kp}}
\textbf{$\eta$ and $\omega$ Production in Hadronic $Z^0$ Decays}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4823664}{4823664}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett. B528 (2002) 19-33
  \item hep-ex/0201012
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent The production of $\eta$ and $\omega$ mesons measured using 4 millon $Z^0$ events by the ALEPH experiment at LEP. Only the fragmentation functions are implemented.

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\clearpage

\typeout{Handling analysis ALEPH_2004_S5765862}\subsection[ALEPH\_2004\_S5765862]{ALEPH\_2004\_S5765862\,\cite{Heister:2003aj}}
\textbf{Jet rates and event shapes at LEP I and II}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6), (66.5, 66.5), (80.5, 80.5), (86.0, 86.0), (91.5, 91.5), (94.5, 94.5), (98.5, 98.5), (100.0, 100.0), (103.0, 103.0) GeV \newline
\textbf{Experiment:} ALEPH (LEP Run 1 and 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+5765862}{5765862}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C35:457-486,2004
  \item DOI: \href{http://dx.doi.org/10.1140/epjc/s2004-01891-4}{10.1140/epjc/s2004-01891-4}
  \item http://cdsweb.cern.ch/record/690637/files/ep-2003-084.pdf
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^- \to$ jet jet (+ jets)\end{itemize}

\noindent Jet rates, event-shape variables and inclusive charged particle spectra are measured in $e^+ e^-$ collisions at CMS energies between 91 and 209 GeV. The previously published data at 91.2 GeV and 133 GeV have been re-processed and the higher energy data are presented here for the first time. Note that the data have been corrected to include neutrinos.

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\typeout{Handling analysis DELPHI_1995_S3137023}\subsection[DELPHI\_1995\_S3137023]{DELPHI\_1995\_S3137023\,\cite{Abreu:1995qx}}
\textbf{Strange baryon production in $Z$ hadronic decays at Delphi}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} DELPHI (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3137023}{3137023}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z. Phys. C, 67, 543--554 (1995)
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurement of the $\Xi^-$ and $\Sigma^+(1385)/\Sigma^-(1385)$ scaled momentum distributions by DELPHI at LEP 1. The paper also has the production cross-sections of these particles, but that's not implemented in Rivet.

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\typeout{Handling analysis DELPHI_1996_S3430090}\subsection[DELPHI\_1996\_S3430090]{DELPHI\_1996\_S3430090\,\cite{Abreu:1996na}}
\textbf{Delphi MC tuning on event shapes and identified particles.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} DELPHI (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3430090}{3430090}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys.C73:11-60,1996
  \item DOI: \href{http://dx.doi.org/10.1007/s002880050295}{10.1007/s002880050295}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item \ensuremath{\sqrt{s}} = 91.2 GeV, $e^+ e^- \ensuremath{\to} Z^0$ production with hadronic decays only\end{itemize}

\noindent Event shape and charged particle inclusive distributions measured using 750000 decays of Z bosons to hadrons from the DELPHI detector at LEP. This data, combined with identified particle distributions from all LEP experiments, was used for tuning of shower-hadronisation event generators by the original PROFESSOR method.  This is a critical analysis for MC event generator tuning of final state radiation and both flavour and kinematic aspects of hadronisation models.

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\typeout{Handling analysis DELPHI_1999_S3960137}\subsection[DELPHI\_1999\_S3960137]{DELPHI\_1999\_S3960137\,\cite{Abreu:1998nn}}
\textbf{Measurement of inclusive $\rho^0$, $f_0(980)$, $f_2(1270)$, $K^{*0}_2(1430)$ and $f'_2(1525)$ production in $Z^0$ decays}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} DELPHI (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3960137}{3960137}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B449:364-382,1999
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent DELPHI results for the production of  $\rho^0$, $f_0(980)$, $f_2(1270)$, $K^{*0}_2(1430)$ and $f'_2(1525)$ in $Z^0$ decays. Only the identified particle spectra for $\rho^0$, $f_0(980)$ and $f_2(1270)$ are implemented.

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\typeout{Handling analysis DELPHI_2000_S4328825}\subsection[DELPHI\_2000\_S4328825]{DELPHI\_2000\_S4328825\,\cite{Abreu:2000nt}}
\textbf{Hadronization properties of $b$ quarks compared to light quarks in $e^+e^-\to q \bar q$ from 183 GeV to 200 GeV}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (91.5, 91.5), (94.5, 94.5), (96.0, 96.0), (98.0, 98.0), (100.0, 100.0), (103.0, 103.0) GeV \newline
\textbf{Experiment:} OPAL (LEP 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4328825}{4328825}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B479:118-128,2000
  \item hep-ex/0103022
  \item DELPHI 2002-052 CONF 586
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurements of the mean charged multiplicities separately for $b\bar b$, $c\bar c$ and light quark ($uds$) initiated events in $e^+e^-$ interactions at energies above the $Z^0$ mass. In addition to the energy points in the original paper one additional point at 206 GeV is included from a later preliminary result.

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\typeout{Handling analysis DELPHI_2002_069_CONF_603}\subsection{DELPHI\_2002\_069\_CONF\_603}
\textbf{Study of the b-quark fragmentation function at LEP 1}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} DELPHI (LEP 1)\newline
\textbf{Status:} PRELIMINARY\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item DELPHI note 2002-069-CONF-603 (ICHEP 2002)
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurement of the $b$-quark fragmentation function by DELPHI using 1994 LEP 1 data. The fragmentation function for both weakly decaying and primary $b$-quarks has been determined in a model independent way. Nevertheless the authors trust $f(x_B^\text{weak})$ more than $f(x_B^\text{prim})$.

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\typeout{Handling analysis JADE_OPAL_2000_S4300807}\subsection[JADE\_OPAL\_2000\_S4300807]{JADE\_OPAL\_2000\_S4300807\,\cite{Pfeifenschneider:1999rz}}
\textbf{Jet rates in $e^+e^-$ at JADE [35--44 GeV] and OPAL [91--189 GeV].}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (17.5, 17.5), (22.0, 22.0), (45.6, 45.6), (66.5, 66.5), (80.5, 80.5), (86.0, 86.0), (91.5, 91.5), (94.5, 94.5) GeV \newline
\textbf{Experiment:} JADE_OPAL (PETRA and LEP)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4300807}{4300807}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C17:19-51,2000
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0001055}{hep-ex/0001055}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^- \to$ jet jet (+ jets)\end{itemize}

\noindent Differential and integrated jet rates for Durham and JADE jet algorithms.

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\typeout{Handling analysis OPAL_1993_S2692198}\subsection[OPAL\_1993\_S2692198]{OPAL\_1993\_S2692198\,\cite{Acton:1992jk}}
\textbf{Measurement of photon production at LEP 1}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2692198}{2692198}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys.C58:405-418,1993
  \item DOI: \href{http://dx.doi.org/10.1007/BF01557697}{10.1007/BF01557697}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^- \to$ jet jet (+ photons)\end{itemize}

\noindent Measurement of the production of photons in $e^+ e^-\to q \bar q$ events at LEP 1.

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\typeout{Handling analysis OPAL_1994_S2927284}\subsection[OPAL\_1994\_S2927284]{OPAL\_1994\_S2927284\,\cite{Akers:1994ez}}
\textbf{Measurement of the production rates of charged hadrons in $e^+e^-$ annihilation at the $Z^0$}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2927284}{2927284}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys.C63:181-196,1994
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent The inclusive production rates of $\pi^\pm$, $K^\pm$ and $p\bar{p}$ in $Z^0$ decays measured using the OPAL detector at LEP. Only the differential cross sections are currently implemented.

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\typeout{Handling analysis OPAL_1995_S3198391}\subsection[OPAL\_1995\_S3198391]{OPAL\_1995\_S3198391\,\cite{Alexander:1995gq}}
\textbf{$\Delta^{++}$ Production in Hadronic $Z^0$ Decays}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3198391}{3198391}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B358:162-172,1995
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent The production of $\Delta^{++}$ baryons measured using 3.5 millon $Z^0$ events by the OPAL experiment at LEP. Only the fragmentation function is implemented.

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\typeout{Handling analysis OPAL_1996_S3257789}\subsection[OPAL\_1996\_S3257789]{OPAL\_1996\_S3257789\,\cite{Alexander:1995qb}}
\textbf{$J/\psi$ and $\psi^\prime$ Production in Hadronic $Z^0$ Decays}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3257789}{3257789}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys. C70 (1996) 197-210
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent The production of $J/\psi$ and $\psi^\prime$ mesons measured by the OPAL experiment at LEP. The fragmentation function for $J/\psi$ and the multiplicities of  $J/\psi$ and $\psi^\prime$ are included.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_1997_S3396100}\subsection[OPAL\_1997\_S3396100]{OPAL\_1997\_S3396100\,\cite{Alexander:1996qj}}
\textbf{Strange baryon production in $Z$ hadronic decays at OPAL}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3396100}{3396100}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z. Phys. C, 73, 569--586 (1997)
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurement of the $\Xi^-$, $\Lambda^0$, $\Sigma^+(1385)$, $\Sigma^-(1385)$, $\Xi^0(1530)$ and $\Lambda^0(1520)$ scaled momentum distributions by OPAL at LEP 1. The paper also has the production cross-sections of these particles, but that is not implemented in Rivet.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_1997_S3608263}\subsection[OPAL\_1997\_S3608263]{OPAL\_1997\_S3608263\,\cite{Ackerstaff:1997kj}}
\textbf{$K^{*0}$ meson production measured by OPAL at LEP 1.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3608263}{3608263}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B412:210-224,1997
  \item hep-ex/9708022
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent The $K^{*0}$ fragmentation function has been measured in hadronic $Z^0$ decays. In addition the  helicity density matrix elements for inclusive $K^*(892)^0$ mesons from hadronic $Z^0$ decays have been measured over the full range of $K^{*0}$ momentum using data taken with the OPAL experiment at LEP. Only the fragmentation function measurement is currently implemented.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_1998_S3702294}\subsection[OPAL\_1998\_S3702294]{OPAL\_1998\_S3702294\,\cite{Ackerstaff:1998ue}}
\textbf{Production of $f_0(980)$, $f_2(1270)$ and $\phi(1020)$ in hadronic $Z^0$ decay}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3702294}{3702294}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C4:19-28,1998
  \item hep-ex/9802013
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Inclusive production of the $f_0(980)$, $f_2(1270)$ and $\phi(1020)$ resonances studied in a sample of 4.3 million hadronic $Z^0$ decays from the OPAL experiment at LEP. Fragmentation functions are reported for the three states.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_1998_S3749908}\subsection[OPAL\_1998\_S3749908]{OPAL\_1998\_S3749908\,\cite{Ackerstaff:1998ap}}
\textbf{Photon and Light Meson Production in Hadronic $Z^0$ Decays}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3749908}{3749908}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C5:411-437,1998
  \item hep-ex/9805011
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent The inclusive production rates and differential cross sections of photons and mesons with a final state containing photons have been measured with the OPAL detector at LEP. The light mesons covered by the measurements are the $\pi^0$, $\eta$, $\rho(770)^\pm$, $\omega(782)$, $\eta'(958)$ and $a_0(980)^\pm$.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_1998_S3780481}\subsection[OPAL\_1998\_S3780481]{OPAL\_1998\_S3780481\,\cite{Ackerstaff:1998hz}}
\textbf{Measurements of flavor dependent fragmentation functions in $Z^0 \ensuremath{\to} q \bar{q}$ events}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3780481}{3780481}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur. Phys. J, C7, 369--381 (1999)
  \item hep-ex/9807004
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurement of scaled momentum distributions and total charged multiplicities in flavour tagged events at LEP 1. OPAL measured these observables in uds-, c-, and b-events separately. An inclusive measurement is also included.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_2000_S4418603}\subsection[OPAL\_2000\_S4418603]{OPAL\_2000\_S4418603\,\cite{Abbiendi:2000cv}}
\textbf{Multiplicities of $\pi^0$, $\eta$, $K^0$ and of charged particles in quark and gluon jets}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4418603}{4418603}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C17:373-387,2000
  \item hep-ex/0007017
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Multiplicities of $\pi^0$, $\eta$, $K^0$ and of charged particles in quark and gluon jets in 3-jet events, as measured by the OPAL experiment at LEP. The main implemented measurement is the $K^0$ fragmentation function.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_2001_S4553896}\subsection[OPAL\_2001\_S4553896]{OPAL\_2001\_S4553896\,\cite{Abbiendi:2001qn}}
\textbf{Four-jet angles using Durham algorithm}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} OPAL (LEP Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4553896}{4553896}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C20:601-615,2001
  \item DOI: \href{http://dx.doi.org/10.1007/s100520100699}{10.1007/s100520100699}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0101044}{hep-ex/0101044}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV) Hadronisation should be turned off because the data is corrected back to the parton level.\end{itemize}

\noindent Angles between the leading (in energy) four jets defined using the Durham algorithm with $y_\mathrm{cut}=0.008$. The data is presented at the parton level and includes the Bengtsson-Zerwas, Korner-Schierholz-Willrodt and Nachtmann-Reiter angles as well as the angle between the two softest jets.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_2002_S5361494}\subsection[OPAL\_2002\_S5361494]{OPAL\_2002\_S5361494\,\cite{Abbiendi:2002vn}}
\textbf{Charged particle multiplicities in heavy and light quark initiated events above the $Z^0$ peak}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (65.0, 65.0), (68.0, 68.0), (80.5, 80.5), (86.0, 86.0), (91.5, 91.5), (94.5, 94.5), (96.0, 96.0), (98.0, 98.0), (100.0, 100.0), (101.0, 101.0), (103.0, 103.0) GeV \newline
\textbf{Experiment:} OPAL (LEP 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+5361494}{5361494}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett. B550 (2002) 33-46
  \item hep-ex/0211007
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurements of the mean charged multiplicities separately for $b\bar b$, $c\bar c$ and light quark ($uds$) initiated events in $e^+e^-$ interactions at energies above the $Z^0$ mass. The data is from the LEP running periods between 1995 and 2000.

\clearpage


\clearpage

\typeout{Handling analysis OPAL_2004_S6132243}\subsection[OPAL\_2004\_S6132243]{OPAL\_2004\_S6132243\,\cite{Abbiendi:2004qz}}
\textbf{Event shape distributions and moments in $e^+ e^-$ \ensuremath{\to} hadrons at 91--209 GeV}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6), (66.5, 66.5), (88.5, 88.5), (98.5, 98.5) GeV \newline
\textbf{Experiment:} OPAL (LEP 1 \& 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6132243}{6132243}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C40:287-316,2005
  \item hep-ex/0503051
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic $e^+ e^-$ events at 4 representative energies (91, 133, 177, 197). Runs need to have ISR suppressed, since the analysis was done using a cut of $\sqrt{s} - \sqrt{s_\text{reco}} < 1\,\text{GeV}$. Particles with a livetime $> 3 \cdot 10^{-10}\,\text{s}$ are considered to be stable.\end{itemize}

\noindent Measurement of $e^+ e^-$ event shape variable distributions and their 1st to 5th moments in LEP running from the Z pole to the highest LEP 2 energy of 209 GeV.

\clearpage


\clearpage

\typeout{Handling analysis SLD_1996_S3398250}\subsection[SLD\_1996\_S3398250]{SLD\_1996\_S3398250\,\cite{Abe:1996zi}}
\textbf{Charged particle multiplicities in heavy and light quark initiated events on the $Z^0$ peak}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} SLD (SLC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3398250}{3398250}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B386:475-485,1996
  \item hep-ex/9608008
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurements of the mean charged multiplicities separately for $b\bar b$, $c\bar c$ and light quark ($uds$) initiated events in $e^+e^-$ interactions at the $Z^0$ mass.

\clearpage


\clearpage

\typeout{Handling analysis SLD_1999_S3743934}\subsection[SLD\_1999\_S3743934]{SLD\_1999\_S3743934\,\cite{Abe:1998zs}}
\textbf{Production of $\pi^+$, $K^+$, $K^0$, $K^{*0}$, $\Phi$, $p$ and $\Lambda^0$ in hadronic $Z^0$ decay}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} SLD (SLC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3743934}{3743934}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D59:052001,1999
  \item hep-ex/9805029
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurement of scaled momentum distributions and fragmentation functions in flavour tagged events at SLC. SLD measured these observables in uds-, c-, and b-events separately. An inclusive measurement is also included.

\clearpage


\clearpage

\typeout{Handling analysis SLD_2002_S4869273}\subsection[SLD\_2002\_S4869273]{SLD\_2002\_S4869273\,\cite{Abe:2002iq}}
\textbf{Measurement of the b-quark fragmentation function in $Z^0$ decays}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} SLD (SLC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4869273}{4869273}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rev.D65:092006,2002
  \item hep-ex/0202031
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurement of the $b$-quark fragmentation function by SLC. The fragmentation function for weakly decaying $b$-quarks has been measured.

\clearpage


\clearpage

\typeout{Handling analysis SLD_2004_S5693039}\subsection[SLD\_2004\_S5693039]{SLD\_2004\_S5693039\,\cite{Abe:2003iy}}
\textbf{Production of $\pi^+$, $\pi^-$, $K^+$, $K^-$, $p$ and $\bar p$ in Light ($uds$), $c$ and $b$ Jets from Z Decays}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (45.6, 45.6) GeV \newline
\textbf{Experiment:} SLD (SLC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+5693039}{5693039}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D69:072003,2004
  \item hep-ex/0310017
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic Z decay events generated on the Z pole (\ensuremath{\sqrt{s}} = 91.2 GeV)\end{itemize}

\noindent Measurements of the differential production rates of stable charged particles in hadronic $Z^0$ decays, and of charged pions, kaons and protons identified over a wide momentum range. In addition to flavour-inclusive $Z^0$ decays, measurements are made for $Z^0$ decays into light ($u$, $d$, $s$), $c$ and $b$ primary flavors.

\clearpage


\section{Tevatron analyses}\typeout{Handling analysis CDF_1988_S1865951}\subsection[CDF\_1988\_S1865951]{CDF\_1988\_S1865951\,\cite{Abe:1988yu}}
\textbf{CDF transverse momentum distributions at 630 GeV and 1800 GeV.}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (315.0, 315.0), (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run I)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1865951}{1865951}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant@durham.ac.uk}{c.l.j.j.vaillant@durham.ac.uk}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.61:1819,1988
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.61.1819}{10.1103/PhysRevLett.61.1819}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD min bias events at \ensuremath{\sqrt{s}} = 630 GeV and 1800 GeV, $|\eta| < 1.0$.\end{itemize}

\noindent Transverse momentum distributions at 630 GeV and 1800 GeV based on data from the CDF experiment at the Tevatron collider.

\clearpage


\clearpage

\typeout{Handling analysis CDF_1990_S2089246}\subsection[CDF\_1990\_S2089246]{CDF\_1990\_S2089246\,\cite{Abe:1989td}}
\textbf{CDF pseudorapidity distributions at 630 and 1800 GeV}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (315.0, 315.0), (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 0)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2089246}{2089246}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D41:2330,1990
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.41.2330}{10.1103/PhysRevD.41.2330}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD min bias events at \ensuremath{\sqrt{s}} = 630 and 1800 GeV. Particles with $c \tau > 10$mm should be set stable.\end{itemize}

\noindent Pseudorapidity distributions based on the CDF 630 and 1800 GeV runs from 1987. All data is detector corrected. The data confirms the UA5 measurement of a $\d{N}/\d{\eta}$ rise with energy faster than $\ln{\sqrt{s}}$, and as such this analysis is important for constraining the energy evolution of minimum bias and underlying event characteristics in MC simulations.

\clearpage


\clearpage

\typeout{Handling analysis CDF_1994_S2952106}\subsection[CDF\_1994\_S2952106]{CDF\_1994\_S2952106\,\cite{Abe:1994nj}}
\textbf{CDF Run I color coherence analysis.}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2952106}{2952106}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lars Sonnenschein $\langle\,$\href{mailto:Lars.Sonnenschein@cern.ch}{Lars.Sonnenschein@cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D50,5562,1994
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.50.5562}{10.1103/PhysRevD.50.5562}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events at \ensuremath{\sqrt{s}} = 1800 GeV. Leading jet \pTmin = 100 GeV.\end{itemize}

\noindent CDF Run I color coherence analysis. Events with $\ge 3$ jets are selected and Et distributions of the three highest-\pT jets are obtained. The plotted quantities are the $\Delta{R}$ between the 2nd and 3rd leading jets in the \pT and pseudorapidity of the 3rd jet, and $\alpha = \mathrm{d}{\eta}/\mathrm{d}{\phi}$, where $\mathrm{d}{\eta}$ is the pseudorapidity difference between the 2nd and 3rd jets and $\mathrm{d}{\phi}$ is their azimuthal angle difference.  Since the data has not been detector-corrected, a bin by bin correction is applied, based on the distributions with ideal and CDF simulation as given in the publication.

\clearpage


\clearpage

\typeout{Handling analysis CDF_1996_S3418421}\subsection[CDF\_1996\_S3418421]{CDF\_1996\_S3418421\,\cite{Abe:1996mj}}
\textbf{Dijet angular distributions}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3418421}{3418421}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.77:5336-5341,1996
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.77.5336}{10.1103/PhysRevLett.77.5336}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/9609011}{hep-ex/9609011}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD dijet events at Tevatron $\sqrt{s}=1.8$ TeV without MPI.\end{itemize}

\noindent Measurement of jet angular distributions in events with two jets in the final state in 5 bins of dijet invariant mass. Based on $106 \mathrm{pb}^{-1}$

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\typeout{Handling analysis CDF_1998_S3618439}\subsection[CDF\_1998\_S3618439]{CDF\_1998\_S3618439\,\cite{Abe:1997eua}}
\textbf{Differential cross-section for events with large total transverse energy}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3618439}{3618439}\newline
\textbf{Status:} UNVALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.80:3461-3466,1998
  \item 10.1103/PhysRevLett.80.3461
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events at Tevatron with $\sqrt{s}=1.8$ TeV without MPI.\end{itemize}

\noindent Measurement of the differential cross section $\mathrm{d}\sigma/\mathrm{d}E_\perp^j$ for the production of multijet events in $p\bar{p}$ collisions where the sum is over all jets with transverse energy $E_\perp^j > E_\perp^\mathrm{min}$.

\clearpage


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\typeout{Handling analysis CDF_2000_S4155203}\subsection[CDF\_2000\_S4155203]{CDF\_2000\_S4155203\,\cite{Affolder:1999jh}}
\textbf{Z \pT measurement in CDF Z \ensuremath{\to} $e^+e^-$ events}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4155203}{4155203}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.84:845-850,2000
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0001021}{hep-ex/0001021}
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.84.845}{10.1103/PhysRevLett.84.845}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ collisions at 1800 GeV. $Z/\gamma^*$ Drell-Yan events with $e^+e^-$ decay mode only. Restrict $Z/\gamma^*$ mass range to roughly $50~\text{GeV}/c^2 < m_{ee} < 120~\text{GeV}/c^2$ for efficiency.\end{itemize}

\noindent Measurement of transverse momentum and total cross section of $e^+e^-$ pairs in the Z-boson region of $66~\text{GeV}/c^2 < m_{ee} < 116~\text{GeV}/c^2$ from pbar-p collisions at \ensuremath{\sqrt{s}} = 1.8 TeV, with the Tevatron CDF detector.  The Z \pT, in a fully-factorised picture, is generated by the momentum balance against initial state radiation (ISR) and the primordial/intrinsic \pT of the Z's parent partons in the incoming hadrons. The Z \pT is important in generator tuning to fix the interplay of ISR and multi-parton interactions (MPI) ingenerating `underlying event' activity.
This analysis is subject to ambiguities in the experimental Z \pT definition, since the Rivet implementation reconstructs the Z momentum from the dilepton pair with finite cones for QED bremstrahlung summation, rather than non-portable direct use of the (sometimes absent) Z in the event record.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2000_S4266730}\subsection[CDF\_2000\_S4266730]{CDF\_2000\_S4266730\,\cite{Affolder:1999ua}}
\textbf{Differential Dijet Mass Cross Section}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4266730}{4266730}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D61:091101,2000
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.61.091101}{10.1103/PhysRevD.61.091101}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/9912022}{hep-ex/9912022}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV\end{itemize}

\noindent Measurement of the cross section for production of two or more jets as a function of dijet mass in the range 180 to 1000 GeV. It is based on an integrated luminosity of $86 \mathrm{pb}^{-1}$.

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\clearpage

\typeout{Handling analysis CDF_2001_S4517016}\subsection[CDF\_2001\_S4517016]{CDF\_2001\_S4517016\,\cite{Affolder:2000ew}}
\textbf{Two jet triply-differential cross-section}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4517016}{4517016}\newline
\textbf{Status:} UNVALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D64:012001,2001
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.64.012001}{10.1103/PhysRevD.64.012001}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0012013}{hep-ex/0012013}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV\end{itemize}

\noindent A measurement of the two-jet differential cross section, $\mathrm{d}^3\sigma/\mathrm{d}E_T \, \mathrm{d}\eta_1 \, \mathrm{d}\eta_2$, based on an integrated luminosity of $86 \mathrm{pb}^{-1}$. The differential cross section is measured as a function of the transverse energy, $E_\perp$, of a jet in the pseudorapidity region $0.1 < |\eta_1| < 0.7$ for four different pseudorapidity bins of a second jet restricted to $0.1 < |\eta_2| < 3.0$.

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\clearpage

\typeout{Handling analysis CDF_2001_S4563131}\subsection[CDF\_2001\_S4563131]{CDF\_2001\_S4563131\,\cite{Affolder:2001fa}}
\textbf{Inclusive jet cross section}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4563131}{4563131}\newline
\textbf{Status:} UNVALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D64:032001,2001
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.64.032001}{10.1103/PhysRevD.64.032001}
  \item arXiv: \href{http://arxiv.org/abs/hep-ph/0102074}{hep-ph/0102074}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Dijet events at Tevatron with $\sqrt{s}=1.8$ TeV\end{itemize}

\noindent Measurement of the inclusive jet cross section for jet transverse energies from 40 to 465 GeV in the pseudo-rapidity range $0.1<|\eta|<0.7$. The results are based on 87 $\mathrm{pb}^{-1}$ of data.

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\clearpage

\typeout{Handling analysis CDF_2001_S4751469}\subsection[CDF\_2001\_S4751469]{CDF\_2001\_S4751469\,\cite{Affolder:2001xt}}
\textbf{Field \& Stuart Run I underlying event analysis.}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4751469}{4751469}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D65:092002,2002
  \item FNAL-PUB 01/211-E
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ QCD interactions at 1800 GeV. The leading jet is binned from 0--49 GeV, and histos can usually can be filled with a single generator run without kinematic sub-samples.\end{itemize}

\noindent The original CDF underlying event analysis, based on decomposing each event into a transverse structure with ``toward'', ``away'' and ``transverse'' regions defined relative to the azimuthal direction of the leading jet in the event. Since the toward region is by definition dominated by the hard process, as is the away region by momentum balance in the matrix element, the transverse region is most sensitive to multi-parton interactions. The transverse regions occupy $|\phi| \in [60\degree, 120\degree]$ for $|\eta| < 1$. The \pT ranges for the leading jet are divided experimentally into the `min-bias' sample from 0--20 GeV, and the `JET20' sample from 18--49 GeV.

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\typeout{Handling analysis CDF_2002_S4796047}\subsection[CDF\_2002\_S4796047]{CDF\_2002\_S4796047\,\cite{Acosta:2001rm}}
\textbf{CDF Run 1 charged multiplicity measurement}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (315.0, 315.0), (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4796047}{4796047}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D65:072005,2002
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.65.072005}{10.1103/PhysRevD.65.072005}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events at \ensuremath{\sqrt{s}} = 630 and 1800 GeV.\end{itemize}

\noindent A study of $p\bar{p}$ collisions at \ensuremath{\sqrt{s}} = 1800 and 630 GeV collected using a minimum bias trigger in which the data set is divided into two classes corresponding to `soft' and `hard' interactions. For each subsample, the analysis includes measurements of the multiplicity, transverse momentum (\pT) spectra, and the average \pT and event-by-event \pT dispersion as a function of multiplicity. A comparison of results shows distinct differences in the behavior of the two samples as a function of the center of mass energy. The properties of the soft sample are invariant as a function of c.m. energy.
It should be noticed that minimum bias tunings of PYTHIA made by ATLAS in early 2010, which used this among all other available data from CDF and from ATLAS at 900~GeV and 7~TeV, found an unavoidable tension between this data and the rest. Accordingly, this data was excluded from the fits. Whether this reflects a problem with this dataset or with the PYTHIA MPI model is a judgement for users to make!

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\typeout{Handling analysis CDF_2004_S5839831}\subsection[CDF\_2004\_S5839831]{CDF\_2004\_S5839831\,\cite{Acosta:2004wqa}}
\textbf{Transverse cone and `Swiss cheese' underlying event studies}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (315.0, 315.0), (900.0, 900.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+5839831}{5839831}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rev. D70, 072002 (2004)
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0404004}{hep-ex/0404004}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events at \ensuremath{\sqrt{s}} = 630 \& 1800 GeV. Several \pTmin cutoffs are probably required to fill the profile histograms, e.g. 0 (min bias), 30, 90, 150 GeV at 1800 GeV, and 0 (min bias), 20, 90, 150 GeV at 630 GeV.\end{itemize}

\noindent This analysis studies the underlying event via transverse cones of  $R = 0.7$ at 90 degrees in \phi relative to the leading (highest E) jet, at \ensuremath{\sqrt{s}} = 630 and 1800 GeV. This is similar to the 2001 CDF UE analysis, except that cones, rather than the whole central \eta range are used. The transverse cones are categorised as TransMIN and TransMAX on an event-by-event basis, to give greater sensitivity to the UE component.
`Swiss Cheese' distributions, where cones around the leading $n$ jets are excluded from the distributions, are also included for $n = 2, 3$.  This analysis is useful for constraining the energy evolution of the underlying event, since it performs the same analyses at two distinct CoM energies.
WARNING! The \pT plots are normalised to raw number of events. The min bias data have not been reproduced by MC, and are not recommended for tuning.

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\typeout{Handling analysis CDF_2005_S6080774}\subsection[CDF\_2005\_S6080774]{CDF\_2005\_S6080774\,\cite{Acosta:2004sn}}
\textbf{Differential cross sections for prompt diphoton production}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6080774}{6080774}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rev. Lett. 95, 022003
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.95.022003}{10.1103/PhysRevLett.95.022003}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0412050}{hep-ex/0412050}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to \gamma \gamma$ [+ jets] at 1960 GeV. The analysis uses photons with \pT larger then 13 GeV. To allow for shifts in the shower, the ME cut on the transverse photon momentum shouldn't be too hard, e.g. 5 GeV.\end{itemize}

\noindent Measurement of the cross section of prompt diphoton production in $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV using a data sample of 207~pb$^{-1}$ as a function of the diphoton mass, the transverse momentum of the diphoton system, and the azimuthal angle between the two photons.

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\typeout{Handling analysis CDF_2005_S6217184}\subsection[CDF\_2005\_S6217184]{CDF\_2005\_S6217184\,\cite{Acosta:2005ix}}
\textbf{CDF Run II jet shape analysis}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6217184}{6217184}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lars Sonnenschein $\langle\,$\href{mailto:Lars.Sonnenschein@cern.ch}{Lars.Sonnenschein@cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D71:112002,2005
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.71.112002}{10.1103/PhysRevD.71.112002}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0505013}{hep-ex/0505013}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events at \ensuremath{\sqrt{s}} = 1960 GeV. Jet \pTmin in plots is 37 GeV/c --- choose generator min \pT somewhere well below this.\end{itemize}

\noindent Measurement of jet shapes in inclusive jet production in p pbar collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. The data cover jet transverse momenta from 37--380 GeV and absolute jet rapidities in the range 0.1--0.7.

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\typeout{Handling analysis CDF_2006_S6450792}\subsection[CDF\_2006\_S6450792]{CDF\_2006\_S6450792\,\cite{Abulencia:2005yg}}
\textbf{Inclusive jet cross section differential in \pT}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6450792}{6450792}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D74:071103,2006
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.74.071103}{10.1103/PhysRevD.74.071103}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0512020}{hep-ex/0512020}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ \ensuremath{\to} jets at 1960 GeV\end{itemize}

\noindent Measurement of the inclusive jet cross section in ppbar interactions at $\sqrt{s}=1.96$ TeV using 385 $\mathrm{pb}^{-1}$ of data. The data cover the jet transverse momentum range from 61 to 620 GeV/c in $0.1 < |y| < 0.7$. This analysis has been updated with more data in more rapidity bins in CDF_2008_S7828950.

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\typeout{Handling analysis CDF_2006_S6653332}\subsection[CDF\_2006\_S6653332]{CDF\_2006\_S6653332\,\cite{Abulencia:2006ce}}
\textbf{b-jet cross section in Z + jets events}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6653332}{6653332}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lars Sonnenschein $\langle\,$\href{mailto:Lars.Sonnenschein@cern.ch}{Lars.Sonnenschein@cern.ch}$\,\rangle$
  \item Steffen Schumann <s.schumann(at)thphys.uni-heidelberg.de>
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D.74:032008,2006
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.74.032008}{10.1103/PhysRevD.74.032008}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0605099v2}{hep-ex/0605099v2}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Z + jets events at \ensuremath{\sqrt{s}} = 1960 GeV. Jets min \pT cut = 20~GeV, leptons min \pT cut = 10~GeV\end{itemize}

\noindent Measurement of the $b$-jet cross section in events with $Z$ boson in $p\bar{p}$ collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. The data cover jet transverse momenta above 20 GeV and jet pseudorapidities in the range -1.5 to 1.5. $Z$ bosons are identified in their electron and muon decay modes in an invariant dilepton mass range between 66 and 116 GeV.

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\typeout{Handling analysis CDF_2007_S7057202}\subsection[CDF\_2007\_S7057202]{CDF\_2007\_S7057202\,\cite{Abulencia:2007ez}}
\textbf{CDF Run II inclusive jet cross-section using the kT algorithm}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7057202}{7057202}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item David Voong
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D75:092006,2007
  \item Erratum-ibid.D75:119901,2007
  \item FNAL-PUB 07/026-E
  \item hep-ex/0701051
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item p-pbar collisions at 1960~GeV. Jet \pT bins from 54~GeV to 700~GeV. Jet rapidity $< |2.1|$.\end{itemize}

\noindent CDF Run II measurement of inclusive jet cross sections at a p-pbar collision energy of 1.96~TeV. Jets are reconstructed in the central part of the detector ($|y|<2.1$) using the kT algorithm with an $R$ parameter of 0.7. The minimum jet \pT considered is 54~GeV, with a maximum around 700~GeV.  The inclusive jet \pT is plotted in bins of rapidity $|y|<0.1$, $0.1<|y|<0.7$, $0.7<|y|<1.1$, $1.1<|y|<1.6$ and $1.6<|y|<2.1$.

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\typeout{Handling analysis CDF_2008_LEADINGJETS}\subsection{CDF\_2008\_LEADINGJETS}
\textbf{CDF Run 2 underlying event in leading jet events}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+NONE}{NONE}\newline
\textbf{Status:} OBSOLETE\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ QCD interactions at 1960~GeV. Particles with $c \tau > {}$10 mm should be set stable. Several $p_\perp^\text{min}$ cutoffs are probably required to fill the profile histograms. $p_\perp^\text{min} = {}$ 0 (min bias), 10, 20, 50, 100, 150 GeV. The corresponding merging points are at $p_T = $ 0, 30, 50, 80, 130, 180 GeV\end{itemize}

\noindent Rick Field's measurement of the underlying event in leading jet events. If the leading jet of the event is within $|\eta| < 2$, the event is accepted and ``toward'', ``away'' and ``transverse'' regions are defined in the same way as in the original (2001) CDF underlying event analysis. The leading jet defines the $\phi$ direction of the toward region. The transverse regions are most sensitive to the underlying event.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2008_NOTE_9351}\subsection{CDF\_2008\_NOTE\_9351}
\textbf{CDF Run 2 underlying event in Drell-Yan}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+NONE}{NONE}\newline
\textbf{Status:} OBSOLETE\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CDF public note 9351
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item ppbar collisions at 1960 GeV.
  \item Drell-Yan events with $Z/\gamma* \ensuremath{\to} e e$ and $Z/\gamma* \ensuremath{\to} \mu\mu$.
  \item A mass cut $m_{ll} > 70~\text{GeV}$ can be applied on generator level.
  \item Particles with $c \tau > 10~\text{mm}$ should be set stable.\end{itemize}

\noindent Deepak Kar and Rick Field's measurement of the underlying event in Drell-Yan events. $Z \ensuremath{\to} ee$ and $Z \ensuremath{\to} \mu\mu$ events are selected using a $Z$ mass window cut between 70 and 110~GeV. ``Toward'', ``away'' and ``transverse'' regions are defined in the same way as in the original (2001) CDF underlying event analysis. The reconstructed $Z$ defines the $\phi$ direction of the toward region. The leptons are ignored after the $Z$ has been reconstructed. Thus the region most sensitive to the underlying event is the toward region (the recoil jet is boosted into the away region).

\clearpage


\clearpage

\typeout{Handling analysis CDF_2008_S7540469}\subsection[CDF\_2008\_S7540469]{CDF\_2008\_S7540469\,\cite{:2007cp}}
\textbf{Measurement of differential Z/$\gamma^*$ + jet + X cross sections}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7540469}{7540469}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.100:102001,2008
  \item arXiv: \href{http://arxiv.org/abs/0711.3717}{0711.3717}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to e^+ e^-$ + jets at 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $66 < m_{ee} < 116$\end{itemize}

\noindent Cross sections as a function of jet transverse momentum in 1 and 2 jet events, and jet multiplicity in ppbar collisions at \ensuremath{\sqrt{s}} = 1.96 TeV, based on an integrated luminosity of $1.7~\text{fb}^{-1}$. The measurements cover the rapidity region $|y_\text{jet}| < 2.1$ and the transverse momentum range $\pT^\text{jet} > 30~\text{GeV}/c$.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2008_S7828950}\subsection[CDF\_2008\_S7828950]{CDF\_2008\_S7828950\,\cite{Aaltonen:2008eq}}
\textbf{CDF Run II inclusive jet cross-section using the Midpoint algorithm}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7828950}{7828950}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Craig Group $\langle\,$\href{mailto:group@fnal.gov}{group@fnal.gov}$\,\rangle$
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0807.2204}{0807.2204}
  \item Phys.Rev.D78:052006,2008
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Requires $2\rightarrow{2}$ QCD scattering processes. The minimum jet $E_\perp$ is 62 GeV, so a cut on kinematic \pTmin may be required for good statistics.\end{itemize}

\noindent Measurement of the inclusive jet cross section in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV as a function of jet $E_\perp$, for $E_\perp >$ 62 GeV. The data is collected by the CDF II detector and has an integrated luminosity of 1.13 fb$^{-1}$. The measurement was made using the cone-based Midpoint jet clustering algorithm in rapidity bins within $|y|<2.1$. This measurement can be used to provide increased precision in PDFs at high parton momentum fraction $x$.

\clearpage


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\typeout{Handling analysis CDF_2008_S8093652}\subsection[CDF\_2008\_S8093652]{CDF\_2008\_S8093652\,\cite{Aaltonen:2008dn}}
\textbf{Dijet mass spectrum}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8093652}{8093652}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0812.4036}{0812.4036}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to$ jets at 1960 GeV\end{itemize}

\noindent Dijet mass spectrum  from 0.2 TeV to 1.4 TeV in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 1.13 fb$^{-1}$.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2008_S8095620}\subsection[CDF\_2008\_S8095620]{CDF\_2008\_S8095620\,\cite{Aaltonen:2008mt}}
\textbf{CDF Run II Z+b-jet cross section paper, 2 fb-1}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8095620}{8095620}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Emily Nurse $\langle\,$\href{mailto:nurse@hep.ucl.ac.uk}{nurse@hep.ucl.ac.uk}$\,\rangle$
  \item Steffen Schumann <s.schumann(at)thphys.uni-heidelberg.de>
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0812.4458}{0812.4458}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Requires the process $p\bar{p} \rightarrow {Z} \rightarrow{\ell}\ell$, where $\ell$ is $e$ or $\mu$. Additional hard jets will also have to be included to get a good description.\end{itemize}

\noindent Measurement of the b-jet production cross section for events containing a $Z$ boson produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV, using data corresponding to an integrated luminosity of 2 fb$^{-1}$ collected by the CDF II detector at the Tevatron. $Z$ bosons are selected in the electron and muon decay modes. Jets are considered with transverse energy $E_T>20$ GeV and pseudorapidity $|\eta|<1.5$. The ratio of the integrated $Z$ + b-jet cross section to the inclusive $Z$ production cross section is measured differentially in jet $E_T$, jet $\eta$, $Z$-boson transverse momentum, number of jets, and number of b-jets. The first two measurements have an entry for each b-jet in the event, the last three measurements have one entry per event.

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\typeout{Handling analysis CDF_2009_NOTE_9936}\subsection{CDF\_2009\_NOTE\_9936}
\textbf{CDF Run 2 min bias charged multiplicity analysis}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+None}{None}\newline
\textbf{Status:} PRELIMINARY\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CDF public note 9936
  \item http://www-cdf.fnal.gov/physics/new/qcd/minbias_mult09/multpage.html
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ QCD interactions at 1960~GeV. Particles with $c \\tau > {}$10 mm should be set stable.\end{itemize}

\noindent Niccolo Moggi's min bias analysis. Minimum bias events are used to measure the charged multiplicity distribution. The multiplicity distribution was not published in S8233977 but the numbers and a public note are available from the CDF website given above. Note: the systematic and statistical errors in Rivet were added in quadrature.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2009_S8233977}\subsection[CDF\_2009\_S8233977]{CDF\_2009\_S8233977\,\cite{Aaltonen:2009ne}}
\textbf{CDF Run 2 min bias cross-section analysis}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8233977}{8233977}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
  \item Niccolo' Moggi $\langle\,$\href{mailto:niccolo.moggi@bo.infn.it}{niccolo.moggi@bo.infn.it}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D79:112005,2009
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.79.112005}{10.1103/PhysRevD.79.112005}
  \item arXiv: \href{http://arxiv.org/abs/0904.1098}{0904.1098}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ QCD interactions at 1960~GeV. Particles with $c \\tau > {}$10 mm should be set stable.\end{itemize}

\noindent Niccolo Moggi's min bias analysis. Minimum bias events are used to measure the average track \pT vs. charged multiplicity, a track \pT distribution and an inclusive $\sum E_T$ distribution.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2009_S8383952}\subsection[CDF\_2009\_S8383952]{CDF\_2009\_S8383952\,\cite{Aaltonen:2009pc}}
\textbf{Z rapidity measurement}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8383952}{8383952}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0908.3914}{0908.3914}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to e^+ e^-$ + jets at 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $66 < m_{ee} < 116$ GeV\end{itemize}

\noindent CDF measurement of the total cross section and rapidity distribution, $\mathrm{d}\sigma/\mathrm{d}y$, for $q\bar{q}\to \gamma^{*}/Z\to e^{+}e^{-}$ events in the $Z$ boson mass region ($66<M_{ee}<116$ GeV/c$^2$) produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV with 2.1 fb$^{-1}$ of integrated luminosity.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2009_S8436959}\subsection[CDF\_2009\_S8436959]{CDF\_2009\_S8436959\,\cite{Aaltonen:2009ty}}
\textbf{Measurement of the inclusive isolated prompt photon cross-section}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8436959}{8436959}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0910.3623}{0910.3623}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $\gamma$ + jet processes in ppbar collisions at $\sqrt{s} = 1960$~GeV. Minimum \pT cut on the photon in the analysis is 30~GeV.\end{itemize}

\noindent A measurement of the cross section for the inclusive production of isolated photons. The measurement covers the pseudorapidity region $|\eta^\gamma|<1.0$ and the transverse energy range $E_T^\gamma>30$~GeV and is based on 2.5~fb$^{-1}$ of integrated luminosity. The cross section is measured differential in $E_\perp(\gamma)$.

\clearpage


\clearpage

\typeout{Handling analysis CDF_2010_S8591881_DY}\subsection{CDF\_2010\_S8591881\_DY}
\textbf{CDF Run 2 underlying event in Drell-Yan}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8591881}{8591881}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D82:034001,2010
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item ppbar collisions at 1960 GeV.
  \item Drell-Yan events with $Z/\gamma* \ensuremath{\to} e e$ and $Z/\gamma* \ensuremath{\to} \mu\mu$.
  \item A mass cut $m_{ll} > 70~\text{GeV}$ can be applied on generator level.
  \item Particles with $c \tau > 10~\text{mm}$ should be set stable.\end{itemize}

\noindent Deepak Kar and Rick Field's measurement of the underlying event in Drell-Yan events. $Z \ensuremath{\to} ee$ and $Z \ensuremath{\to} \mu\mu$ events are selected using a $Z$ mass window cut between 70 and 110~GeV. ``Toward'', ``away'' and ``transverse'' regions are defined in the same way as in the original (2001) CDF underlying event analysis. The reconstructed $Z$ defines the $\phi$ direction of the toward region. The leptons are ignored after the $Z$ has been reconstructed. Thus the region most sensitive to the underlying event is the toward region (the recoil jet is boosted into the away region).

\clearpage


\clearpage

\typeout{Handling analysis CDF_2010_S8591881_QCD}\subsection{CDF\_2010\_S8591881\_QCD}
\textbf{CDF Run 2 underlying event in leading jet events}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8591881}{8591881}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D82:034001,2010
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ QCD interactions at 1960~GeV. Particles with $c \tau > {}$10 mm should be set stable. Several $p_\perp^\text{min}$ cutoffs are probably required to fill the profile histograms. $p_\perp^\text{min} = {}$ 0 (min bias), 10, 20, 50, 100, 150 GeV. The corresponding merging points are at $p_T = $ 0, 30, 50, 80, 130, 180 GeV\end{itemize}

\noindent Rick Field's measurement of the underlying event in leading jet events. If the leading jet of the event is within $|\eta| < 2$, the event is accepted and ``toward'', ``away'' and ``transverse'' regions are defined in the same way as in the original (2001) CDF underlying event analysis. The leading jet defines the $\phi$ direction of the toward region. The transverse regions are most sensitive to the underlying event.

\clearpage


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\typeout{Handling analysis CDF_2012_NOTE10874}\subsection{CDF\_2012\_NOTE10874}
\textbf{CDF energy scan underlying event analysis}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (150.0, 150.0), (450.0, 450.0), (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron energy scan)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Rick Field $\langle\,$\href{mailto:rfield@phys.ufl.edu}{rfield@phys.ufl.edu}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CDF Note 10874
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p\bar{p}$ QCD interactions at 300, 900, and 1960~GeV. Particles with $c \tau > {}$10 mm should be set stable.\end{itemize}

\noindent In this analysis the behavior of the underlying event in hard scattering proton-antiproton collisions at 300 GeV, 900 GeV, and 1.96 TeV is studied. The 300 GeV and 900 GeV data are a result of the Tevatron Energy Scan which was performed just before the Tevatron was shut down. The energy ratio histograms can be created from different runs with a merging script available in the Rivet bin directory.

\clearpage


\clearpage

\typeout{Handling analysis D0_2000_S4480767}\subsection[D0\_2000\_S4480767]{D0\_2000\_S4480767\,\cite{Abbott:2000xv}}
\textbf{Transverse momentum of the W boson}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4480767}{4480767}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett. B513 (2001) 292-300
  \item DOI: \href{http://dx.doi.org/10.1016/S0370-2693(01)00628-1}{10.1016/S0370-2693(01)00628-1}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0010026}{hep-ex/0010026}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Production of W+ and W- decaying into the electron channel.\end{itemize}

\noindent Measurement of the differential cross section for W boson production as a function of its transverse momentum. The data were collected by the D0 experiment at the Fermilab Tevatron Collider during 1994-1995 and correspond to an integrated luminosity of 85 pb$^{-1}$.

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\clearpage

\typeout{Handling analysis D0_2001_S4674421}\subsection[D0\_2001\_S4674421]{D0\_2001\_S4674421\,\cite{Abazov:2001nta}}
\textbf{Tevatron Run I differential W/Z boson cross-section analysis}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (900.0, 900.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 1)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4674421}{4674421}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lars Sonnenschein $\langle\,$\href{mailto:Lars.Sonnenschein@cern.ch}{Lars.Sonnenschein@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B517:299-308,2001
  \item DOI: \href{http://dx.doi.org/10.1016/S0370-2693(01)01020-6}{10.1016/S0370-2693(01)01020-6}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0107012v2}{hep-ex/0107012v2}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item W/Z events with decays to first generation leptons, in ppbar collisions at \ensuremath{\sqrt{s}} = 1800~GeV\end{itemize}

\noindent Measurement of differential W/Z boson cross section and ratio in $p \bar{p}$ collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.8 TeV. The data cover electrons and neutrinos in a pseudo-rapidity range of -2.5 to 2.5.

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\clearpage

\typeout{Handling analysis D0_2004_S5992206}\subsection[D0\_2004\_S5992206]{D0\_2004\_S5992206\,\cite{Abazov:2004hm}}
\textbf{Run II jet azimuthal decorrelation analysis}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+5992206}{5992206}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lars Sonnenschein $\langle\,$\href{mailto:lars.sonnenschein@cern.ch}{lars.sonnenschein@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rev. Lett., 94, 221801 (2005)
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0409040}{hep-ex/0409040}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events in ppbar interactions at \ensuremath{\sqrt{s}} = 1960 GeV.\end{itemize}

\noindent Correlations in the azimuthal angle between the two largest \pT jets have been measured using the D0 detector in ppbar collisions at 1960~GeV. The analysis is based on an inclusive dijet event sample in the central rapidity region. The correlations are determined for four different \pT intervals.

\clearpage


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\typeout{Handling analysis D0_2006_S6438750}\subsection[D0\_2006\_S6438750]{D0\_2006\_S6438750\,\cite{Abazov:2005wc}}
\textbf{Inclusive isolated photon cross-section, differential in \pT(gamma)}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6438750}{6438750}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Gavin Hesketh $\langle\,$\href{mailto:gavin.hesketh@cern.ch}{gavin.hesketh@cern.ch}$\,\rangle$
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B639:151-158,2006, Erratum-ibid.B658:285-289,2008
  \item DOI: \href{http://dx.doi.org/10.1016/j.physletb.2006.04.048}{10.1016/j.physletb.2006.04.048}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0511054}{hep-ex/0511054}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item ppbar collisions at \ensuremath{\sqrt{s}} = 1960 GeV. Requires gamma + jet (q,qbar,g) hard processes, which for Pythia 6 means MSEL=10 for with MSUB indices 14, 18, 29, 114, 115 enabled.\end{itemize}

\noindent Measurement of differential cross section for inclusive production of isolated photons in p pbar collisions at \ensuremath{\sqrt{s}} = 1.96 TeV with the D\O detector at the Fermilab Tevatron collider. The photons span transverse momenta 23--300 GeV and have pseudorapidity $|\eta| < 0.9$. Isolated direct photons are probes of pQCD via the annihilation ($q \bar{q} \ensuremath{\to} \gamma g$) and quark-gluon Compton scattering ($q g \ensuremath{\to} \gamma q$) processes, the latter of which is also sensitive to the gluon PDF. The initial state radiation / resummation formalisms are sensitive to the resulting photon \pT spectrum

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\typeout{Handling analysis D0_2007_S7075677}\subsection[D0\_2007\_S7075677]{D0\_2007\_S7075677\,\cite{Abazov:2007jy}}
\textbf{$Z/\gamma^* + X$ cross-section shape, differential in $y(Z)$}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7075677}{7075677}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Gavin Hesketh $\langle\,$\href{mailto:ghesketh@fnal.gov}{ghesketh@fnal.gov}$\,\rangle$
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D76:012003,2007
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0702025}{hep-ex/0702025}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Drell-Yan $p \bar{p} \to Z/\gamma^*$ + jets events at $\sqrt{s}$ = 1960 GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than  $71 < m_{ee} < 111$ GeV\end{itemize}

\noindent Cross sections as a function of di-electron rapidity $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$.

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\clearpage

\typeout{Handling analysis D0_2008_S6879055}\subsection[D0\_2008\_S6879055]{D0\_2008\_S6879055\,\cite{Abazov:2006gs}}
\textbf{Measurement of the ratio sigma($Z/\gamma^*$ + $n$ jets)/sigma($Z/\gamma^*$)}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6879055}{6879055}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Giulio Lenzi
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item hep-ex/0608052
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $75 < m_{ee} < 105$ GeV.\end{itemize}

\noindent Cross sections as a function of \pT of the three leading jets and $n$-jet cross section ratios in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$.

\clearpage


\clearpage

\typeout{Handling analysis D0_2008_S7554427}\subsection[D0\_2008\_S7554427]{D0\_2008\_S7554427\,\cite{:2007nt}}
\textbf{$Z/\gamma^* + X$ cross-section shape, differential in $\pT(Z)$}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7554427}{7554427}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0712.0803}{0712.0803}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item * $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV.
  \item Needs mass cut on lepton pair to avoid photon singularity, looser than $40 < m_{ee} < 200$ GeV.\end{itemize}

\noindent Cross sections as a function of \pT of the vector boson inclusive and in forward region ($|y| > 2$, $\pT<30$ GeV) in the di-electron channel in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 0.98~fb$^{-1}$.

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\typeout{Handling analysis D0_2008_S7662670}\subsection[D0\_2008\_S7662670]{D0\_2008\_S7662670\,\cite{:2008hua}}
\textbf{Measurement of D0 Run II differential jet cross sections}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7662670}{7662670}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Gavin Hesketh $\langle\,$\href{mailto:gavin.hesketh@cern.ch}{gavin.hesketh@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.101:062001,2008
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.101.062001}{10.1103/PhysRevLett.101.062001}
  \item arXiv: \href{http://arxiv.org/abs/0802.2400v3}{0802.2400v3}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events at \ensuremath{\sqrt{s}} = 1960 GeV. A \pTmin cut is probably necessary since the lowest jet \pT bin is at 50 GeV\end{itemize}

\noindent Measurement of the inclusive jet cross section in $p \bar{p}$ collisions at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. The data cover jet transverse momenta from 50--600 GeV and jet rapidities in the range -2.4 to 2.4.

\clearpage


\clearpage

\typeout{Handling analysis D0_2008_S7719523}\subsection[D0\_2008\_S7719523]{D0\_2008\_S7719523\,\cite{Abazov:2008er}}
\textbf{Isolated $\gamma$ + jet cross-sections, differential in \pT($\gamma$) for various $y$ bins}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7719523}{7719523}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Gavin Hesketh $\langle\,$\href{mailto:gavin.hesketh@cern.ch}{gavin.hesketh@cern.ch}$\,\rangle$
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B666:435-445,2008
  \item DOI: \href{http://dx.doi.org/10.1016/j.physletb.2008.06.076}{10.1016/j.physletb.2008.06.076}
  \item arXiv: \href{http://arxiv.org/abs/0804.1107v2}{0804.1107v2}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Produce only gamma + jet ($q,\bar{q},g$) hard processes (for Pythia 6, this means MSEL=10 and MSUB indices 14, 29 \& 115 enabled). The lowest bin edge is at 30 GeV, so a kinematic \pTmin cut is probably required to fill the histograms.\end{itemize}

\noindent The process $p \bar{p}$ \ensuremath{\to} photon + jet + X as studied by the D0 detector at the Fermilab Tevatron collider at center-of-mass energy \ensuremath{\sqrt{s}} = 1.96 TeV. Photons are reconstructed in the central rapidity region $|y_\gamma| < 1.0$ with transverse momenta in the range 30--400 GeV, while jets are reconstructed in either the central $|y_\text{jet}| < 0.8$ or forward $1.5 < |y_\text{jet}| < 2.5$ rapidity intervals with $\pT^\text{jet} > 15~\text{GeV}$. The differential cross section $\mathrm{d}^3 \sigma / \mathrm{d}{\pT^\gamma} \mathrm{d}{y_\gamma} \mathrm{d}{y_\text{jet}}$ is measured as a function of $\pT^\gamma$ in four regions, differing by the relative orientations of the photon and the jet.  MC predictions have trouble with simultaneously describing the measured normalization and $\pT^\gamma$ dependence of the cross section in any of the four measured regions.

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\typeout{Handling analysis D0_2008_S7837160}\subsection[D0\_2008\_S7837160]{D0\_2008\_S7837160\,\cite{Abazov:2008qv}}
\textbf{Measurement of W charge asymmetry from D0 Run II}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7837160}{7837160}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Gavin Hesketh $\langle\,$\href{mailto:gavin.hesketh@cern.ch}{gavin.hesketh@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.101:211801,2008
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.101.211801}{10.1103/PhysRevLett.101.211801}
  \item arXiv: \href{http://arxiv.org/abs/0807.3367v1}{0807.3367v1}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item * Event type: W production with decay to $e \, \nu_e$ only
  \item for Pythia 6: MSEL = 12, MDME(206,1) = 1
  \item Energy: 1.96 TeV\end{itemize}

\noindent Measurement of the electron charge asymmetry in $p \bar p \to W + X \to e \nu_e + X$ events at a center of mass energy of 1.96 TeV. The asymmetry is measured as a function of the electron transverse momentum and pseudorapidity in the interval (-3.2, 3.2).  This data is sensitive to proton parton distribution functions due to the valence asymmetry in the incoming quarks which produce the W. Initial state radiation should also affect the \pT distribution.

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\typeout{Handling analysis D0_2008_S7863608}\subsection[D0\_2008\_S7863608]{D0\_2008\_S7863608\,\cite{Abazov:2008ez}}
\textbf{Measurement of differential $Z/\gamma^*$ + jet + $X$ cross sections}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7863608}{7863608}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Gavin Hesketh $\langle\,$\href{mailto:gavin.hesketh@fnal.gov}{gavin.hesketh@fnal.gov}$\,\rangle$
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett. B669 (2008) 278-286
  \item DOI: \href{http://dx.doi.org/10.1016/j.physletb.2008.09.060}{10.1016/j.physletb.2008.09.060}
  \item arXiv: \href{http://arxiv.org/abs/0808.1296}{0808.1296}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to \mu^+ \mu^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{\mu\mu} < 115$ GeV.\end{itemize}

\noindent Cross sections as a function of \pT and rapidity of the boson and \pT and rapidity of the leading jet in the di-muon channel in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 1.0 fb$^{-1}$.

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\clearpage

\typeout{Handling analysis D0_2009_S8202443}\subsection[D0\_2009\_S8202443]{D0\_2009\_S8202443\,\cite{Abazov:2009av}}
\textbf{$Z/\gamma^*$ + jet + $X$ cross sections differential in \pT(jet 1,2,3)}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8202443}{8202443}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0903.1748}{0903.1748}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to e^+ e^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.\end{itemize}

\noindent Cross sections as a function of \pT of the three leading jets in $Z/\gamma^{*} (\to e^{+} e^{-})$ + jet + X production in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 1.0 fb$^{-1}$.

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\typeout{Handling analysis D0_2009_S8320160}\subsection[D0\_2009\_S8320160]{D0\_2009\_S8320160\,\cite{:2009mh}}
\textbf{Dijet angular distributions}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8320160}{8320160}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0906.4819}{0906.4819}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to$ jets at 1960 GeV\end{itemize}

\noindent Dijet angular distributions in different bins of dijet mass from 0.25 TeV to above 1.1 TeV in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 0.7 fb$^{-1}$.

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\clearpage

\typeout{Handling analysis D0_2009_S8349509}\subsection[D0\_2009\_S8349509]{D0\_2009\_S8349509\,\cite{Abazov:2009pp}}
\textbf{Z+jets angular distributions}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8349509}{8349509}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0907.4286}{0907.4286}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to \mu^+ \mu^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{ee} < 115$ GeV.\end{itemize}

\noindent First measurements at a hadron collider of differential cross sections for $Z (\to \mu\mu)$+jet+X production in $\Delta\phi(Z, j)$, $|\Delta y(Z, j)|$ and $|y_\mathrm{boost}(Z, j)|$. Vector boson production in association with jets is an excellent probe of QCD and constitutes the main background to many small cross section processes, such as associated Higgs production. These measurements are crucial tests of the predictions of perturbative QCD and current event generators, which have varied success in describing the data. Using these measurements as inputs in tuning event generators will increase the experimental sensitivity to rare signals.

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\typeout{Handling analysis D0_2010_S8566488}\subsection[D0\_2010\_S8566488]{D0\_2010\_S8566488\,\cite{Abazov:2010fr}}
\textbf{Dijet invariant mass}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8566488}{8566488}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1002.4594}{1002.4594}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to$ jets at 1960 GeV. Analysis needs two hard jets above 40 GeV.\end{itemize}

\noindent The inclusive dijet production double differential cross section as a function of the dijet invariant mass and of the largest absolute rapidity ($|y|_\text{max}$) of the two jets with the largest transverse momentum in an event is measured using 0.7 fb$^{-1}$ of data. The measurement is performed in six rapidity regions up to $|y|_\text{max}=2.4$.

\clearpage


\clearpage

\typeout{Handling analysis D0_2010_S8570965}\subsection[D0\_2010\_S8570965]{D0\_2010\_S8570965\,\cite{Abazov:2010ah}}
\textbf{Direct photon pair production}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} CDF (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8570965}{8570965}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1002.4917}{1002.4917}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item All processes that can produce prompt photon pairs, e.g. $jj \to jj$, $jj \to j\gamma$ and $jj \to \gamma \gamma$. Non-prompt photons from hadron decays like $\pi$ and $\eta$ have been corrected for.\end{itemize}

\noindent Direct photon pair production cross sections are measured using 4.2 fb$^{-1}$ of data. They are binned in diphoton mass, the transverse momentum of the diphoton system, the azimuthal angle between the photons, and the polar scattering angle of the photons. Also available are double differential cross sections considering the last three kinematic variables in three diphoton mass bins. Note, the numbers in version 1 of the arXiv preprint were missing the dM normalisation in the double differential cross sections. This has been reported to and fixed by the authors in v2 and the journal submission. HepData as well as the Rivet analysis have also been updated.

\clearpage


\clearpage

\typeout{Handling analysis D0_2010_S8671338}\subsection[D0\_2010\_S8671338]{D0\_2010\_S8671338\,\cite{Abazov:2010kn}}
\textbf{Measurement of differential $Z/\gamma^*$ \pT}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8671338}{8671338}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Flavia Dias $\langle\,$\href{mailto:fladias@gmail.com}{fladias@gmail.com}$\,\rangle$
  \item Gavin Hesketh $\langle\,$\href{mailto:gavin.hesketh@cern.ch}{gavin.hesketh@cern.ch}$\,\rangle$
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1006.0618}{1006.0618}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $p \bar{p} \to \mu^+ \mu^-$ + jets at 1960~GeV. Needs mass cut on lepton pair to avoid photon singularity, looser than $65 < m_{\mu\mu} < 115$ GeV. Restrict $Z/\gamma^*$ mass range to roughly $50~\text{GeV}/c^2 < m_{\mu\mu} < 120~\text{GeV}/c^2$ for efficiency. Weighted events and kinematic sampling enhancement can help to fill the \pT tail.\end{itemize}

\noindent Cross section as a function of \pT of the Z boson decaying into muons in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 0.97 fb$^{-1}$.

\clearpage


\clearpage

\typeout{Handling analysis D0_2010_S8821313}\subsection[D0\_2010\_S8821313]{D0\_2010\_S8821313\,\cite{Abazov:2010mk}}
\textbf{Precise study of Z \pT using novel technique}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8821313}{8821313}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1010.0262}{1010.0262}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive $Z/\gamma^*$ production in both electron and muon channels. Cut on invariant lepton mass should be wider than $70<m_{\ell\ell}<110$ GeV.\end{itemize}

\noindent Using 7.3 pb-1 the distribution of the variable $\phi^*$ is measured, which probes the same physical effects as the $Z/\gamma^*$ boson transverse momentum, but is less susceptible to the effects of experimental resolution and efficiency. Results are presented for both the di-electron and di-muon channel.

\clearpage


\clearpage

\typeout{Handling analysis D0_2011_I895662}\subsection[D0\_2011\_I895662]{D0\_2011\_I895662\,\cite{Abazov:2011ub}}
\textbf{3-jet invariant mass}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (980.0, 980.0) GeV \newline
\textbf{Experiment:} D0 (Tevatron Run 2)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arxiv:1104.1986
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events, three jets above 40 GeV.\end{itemize}

\noindent Inclusive three-jet differential cross-section as a function of invariant mass of the three jets with the largest transverse momenta. The measurement is made in three rapidity regions ($|y|<0.8, 1.6, 2.4$) and with jets above 40, 70, and 100 GeV.

\clearpage


\section{LHC analyses}\typeout{Handling analysis ALICE_2010_S8624100}\subsection[ALICE\_2010\_S8624100]{ALICE\_2010\_S8624100\,\cite{Aamodt:2010ft}}
\textbf{Charged particle multiplicities at $\unit{0.9 \& 2.36}{\TeV}$ in three different pseudorapidity intervals.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (1180.0, 1180.0) GeV \newline
\textbf{Experiment:} ALICE (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8624100}{8624100}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
  \item Jan Fiete Grosse-Oetringhaus@cern.ch $\langle\,$\href{mailto:Jan.Fiete.Grosse-Oetringhaus@cern.ch}{Jan.Fiete.Grosse-Oetringhaus@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C68:89-108,2010
  \item arXiv: \href{http://arxiv.org/abs/1004.3034}{1004.3034}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD and diffractive events at $\sqrt{s}=\unit{0.9}{\TeV}$ and $\sqrt{s}=\unit{2.36}{\TeV}$\end{itemize}

\noindent This is an ALICE analysis where charged particle multiplicities (including the zero bin) have been measured in three different pseudorapidity intervals ($|\eta|<0.5; |\eta|<1.0; |\eta|<1.3$. Only the INEL distributions have been considered here, i.e. this analysis can only be meaningfully compared to PYTHIA 6 with diffractive processes disabled. The data were taken at 900 and 2360 GeV.

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\clearpage

\typeout{Handling analysis ALICE_2010_S8625980}\subsection[ALICE\_2010\_S8625980]{ALICE\_2010\_S8625980\,\cite{Aamodt:2010pp}}
\textbf{Pseudorapidities at three energies, charged multiplicity at 7 TeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (1180.0, 1180.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ALICE (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8625980}{8625980}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
  \item Jan Fiete Grosse-Oetringhaus@cern.ch $\langle\,$\href{mailto:Jan.Fiete.Grosse-Oetringhaus@cern.ch}{Jan.Fiete.Grosse-Oetringhaus@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J. C68 (2010) 345-354
  \item arXiv: \href{http://arxiv.org/abs/1004.3514}{1004.3514}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Diffractive events need to be enabled.\end{itemize}

\noindent This is an ALICE publication with pseudorapities for $\unit{0.9, 2.36 and 7}{\TeV}$ and the charged multiplicity at $\unit{7}{\TeV}$. The analysis requires at least on charged particle in the event. Only the INEL distributions are considered here

\clearpage


\clearpage

\typeout{Handling analysis ALICE_2010_S8706239}\subsection[ALICE\_2010\_S8706239]{ALICE\_2010\_S8706239\,\cite{Aamodt:2010my}}
\textbf{Charged particle $\langle p_\perp \rangle$ vs. $N_\text{ch}$ in $pp$ collisions at 900 GeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0) GeV \newline
\textbf{Experiment:} ALICE (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8706239}{8706239}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
  \item Jan Fiete Grosse-Oetringhaus@cern.ch $\langle\,$\href{mailto:Jan.Fiete.Grosse-Oetringhaus@cern.ch}{Jan.Fiete.Grosse-Oetringhaus@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B693:53-68,2010
  \item arXiv: \href{http://arxiv.org/abs/1007.0719}{1007.0719}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Diffractive events need to be switched on\end{itemize}

\noindent ALICE measurement of $\langle p_\perp \rangle$ vs. $N_\text{ch}$ and invariant particle yield (as function of $p_\perp$) in proton-proton collisions at $\sqrt{s}=\unit{900}{\GeV}$.

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\clearpage

\typeout{Handling analysis ALICE_2011_S8909580}\subsection[ALICE\_2011\_S8909580]{ALICE\_2011\_S8909580\,\cite{Aamodt:2011zza}}
\textbf{Strange particle production in proton-proton collisions at \ensuremath{\sqrt{s}} = 0.9 TeV with ALICE at the LHC.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0) GeV \newline
\textbf{Experiment:} ALICE (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8909580}{8909580}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Pablo Bueno Gomez $\langle\,$\href{mailto:UO189399@uniovi.es}{UO189399@uniovi.es}$\,\rangle$
  \item Eva Sicking $\langle\,$\href{mailto:esicking@cern.ch}{esicking@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C71:1594,2011.
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Diffractive events need to be switched on.\end{itemize}

\noindent Tranverse momentum spectra of strange particles ($K^0_S$, $\Lambda$, $\phi$ and $\Xi$) in $pp$ collisions at $\sqrt{s} = 0.9$\;TeV with ALICE at the LHC. The ratio of cross-sections as a function of \pT for $\Lambda/K^0_S$ is also included.

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\clearpage

\typeout{Handling analysis ALICE_2011_S8945144}\subsection[ALICE\_2011\_S8945144]{ALICE\_2011\_S8945144\,\cite{Aamodt:2011zj}}
\textbf{Tranverse momentum spectra of pions, kaons and protons in pp collisions at 0.9 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0) GeV \newline
\textbf{Experiment:} ALICE (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8945144}{8945144}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Pablo Bueno Gomez $\langle\,$\href{mailto:UO189399@uniovi.es}{UO189399@uniovi.es}$\,\rangle$
  \item Eva Sicking $\langle\,$\href{mailto:esicking@cern.ch}{esicking@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C71:1655,2011.
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Diffractive events need to be enabled.\end{itemize}

\noindent Obtaining the tranverse momentum spectra of pions, kaons and protons in $pp$ collisions at $\sqrt{s} = 0.9$ TeV with ALICE at the LHC. Mean transverse momentum as a function of the mass of the emitted particle is also included.

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\clearpage

\typeout{Handling analysis ALICE_2012_I1181770}\subsection[ALICE\_2012\_I1181770]{ALICE\_2012\_I1181770\,\cite{:2012sja}}
\textbf{Measurement of inelastic, single- and double-diffraction cross sections in proton--proton collisions at the LHC with ALICE}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (1380.0, 1380.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ALICE (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Martin Poghosyan $\langle\,$\href{mailto:Martin.Poghosyan@cern.ch}{Martin.Poghosyan@cern.ch}$\,\rangle$
  \item Sercan Sen $\langle\,$\href{mailto:Sercan.Sen@cern.ch}{Sercan.Sen@cern.ch}$\,\rangle$
  \item Burak Bilki $\langle\,$\href{mailto:bbilki@gmail.com}{bbilki@gmail.com}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1208.4968}{1208.4968}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inelastic events (non-diffractive and inelastic diffractive).\end{itemize}

\noindent Measurements of cross-sections of inelastic and diffractive processes in proton-proton collisions at $\sqrt{s} = 900$, 2760 and 7000 GeV. The fractions of diffractive processes in inelastic collisions were determined from a study of gaps in charged particle pseudorapidity distributions. Single-diffractive events are selected with $M_{X} < 200\;\GeV/c^2$ and double-diffractive events defined as NSD events with $\Delta\eta > 3$. To measure the inelastic cross-section, beam properties were determined with van der Meer scans using a simulation of diffraction adjusted to data.
Note that these are experimental approximations to theoretical concepts -- it is not totally clear whether the data point values are model-independent.

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\typeout{Handling analysis ATLAS_2010_S8591806}\subsection[ATLAS\_2010\_S8591806]{ATLAS\_2010\_S8591806\,\cite{Aad:2010rd}}
\textbf{Charged particles at 900 GeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 900GeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8591806}{8591806}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1003.3124}{1003.3124}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 900 GeV including diffractive events.\end{itemize}

\noindent The first measurements with the ATLAS detector at the LHC. Data were collected using a minimum-bias trigger in December 2009 during proton-proton collisions at a centre of mass energy of 900 GeV. The charged- particle density, its dependence on transverse momentum and pseudorapid- ity, and the relationship between transverse momentum and charged-particle multiplicity are measured for events with at least one charged particle in the kinematic range $|\eta| < 2.5$ and $p_\perp > 500$ MeV. All data is corrected to the particle level.

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\typeout{Handling analysis ATLAS_2010_S8817804}\subsection[ATLAS\_2010\_S8817804]{ATLAS\_2010\_S8817804\,\cite{Aad:2010wv}}
\textbf{Inclusive jet cross section and di-jet mass and chi spectra at 7 TeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8817804}{8817804}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item James Monk $\langle\,$\href{mailto:jmonk@cern.ch}{jmonk@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1009.5908}{1009.5908}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD jet production with a minimum jet \pT of 60 GeV (inclusive) or 30 GeV (di-jets) at 7 TeV.\end{itemize}

\noindent The first jet cross section measurement made with the ATLAS detector at the LHC. Anti-kt jets with $R=0.4$ and $R=0.6$ are resconstructed within $|y|<2.8$ and above 60~GeV for the inclusive jet cross section plots.  For the di-jet plots the second jet must have \pT>30~GeV. Jet \pT and di-jet mass spectra are plotted in bins or rapidity $|y|<0.3$, $0.3<|y|<0.8$, $0.8<|y|<1.2$, $1.2<|y|<2.1$, $2.1<|y|<2.8$.  Di-jet $\chi$ spectra are plotted in bins of di-jet mass $340~GeV<m_{12}<520~GeV$, $520~GeV<m_{12}<800~GeV$ and $800~GeV<m_{12}<1200~GeV$.

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\typeout{Handling analysis ATLAS_2010_S8894728}\subsection{ATLAS\_2010\_S8894728}
\textbf{Track-based underlying event at 900 GeV and 7 TeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8894728}{8894728}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1012.0791}{1012.0791}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 900 GeV and 7 TeV. Diffractive events should be included, but only influence the lowest bins. Multiple kinematic cuts should not be required.\end{itemize}

\noindent The underlying event measurements with the ATLAS detector at the LHC at the center of mass energies of 900 GeV and 7 TeV. The observables sensitive to the underlying event, i.e the charged particle density and charged \pT sum, as well as their standard deviations and the average \pT, are measured as functions of the leading track. A track \pT cut of 500 MeV is applied for most observables, but the main profile plots are also shown for a lower track cut of 100 MeV, which includes much more of the soft cross-section. The angular distribution of the charged tracks with respect to the leading track is also studied, as are the correlation between mean transverse momentum and charged particle multiplicity, and the `plateau' height as a function of the leading track $|\eta|$.

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\typeout{Handling analysis ATLAS_2010_S8914702}\subsection[ATLAS\_2010\_S8914702]{ATLAS\_2010\_S8914702\,\cite{Collaboration:2010sp}}
\textbf{Inclusive isolated prompt photon analysis}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8914702}{8914702}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Mike Hance $\langle\,$\href{mailto:michael.hance@cern.ch}{michael.hance@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1012.4389}{1012.4389}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive photon+X events (primary gamma+jet events) at $\sqrt{s} = 7$~TeV.\end{itemize}

\noindent A measurement of the cross section for inclusive isolated photon production at $sqrt{s} = 7$ TeV. The measurement covers three ranges in $|\eta|$: [0.00,0.60), [0.60,1.37), and [1.52,1.81), for $E_T^\gamma>15$~GeV.  The measurement uses 880nb$^{-1}$ of integrated luminosity collected with the ATLAS detector.

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\typeout{Handling analysis ATLAS_2010_S8918562}\subsection{ATLAS\_2010\_S8918562}
\textbf{Track-based minimum bias at 900 GeV and 2.36 and 7 TeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (1180.0, 1180.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8918562}{8918562}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Thomas Burgess $\langle\,$\href{mailto:thomas.burgess@cern.ch}{thomas.burgess@cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1012.5104}{1012.5104}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 0.9, 2.36, and 7 TeV. Diffractive events should be included. Multiple kinematic cuts should not be required.\end{itemize}

\noindent Measurements from proton-proton collisions at centre-of-mass energies of \ensuremath{\sqrt{s}} = 0.9, 2.36, and 7 TeV recorded with the ATLAS detector at the LHC. Events were collected using a single-arm minimum-bias trigger. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the relationship between the mean transverse momentum and charged-particle multiplicity are measured. Measurements in different regions of phase-space are shown, providing diffraction-reduced measurements as well as more inclusive ones. The observed distributions are corrected to well-defined phase-space regions, using model-independent corrections.

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\typeout{Handling analysis ATLAS_2010_S8919674}\subsection[ATLAS\_2010\_S8919674]{ATLAS\_2010\_S8919674\,\cite{Aad:2010pg}}
\textbf{W+jets jet multiplicities and \pT}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8919674}{8919674}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1012.5382}{1012.5382}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item W+jets events ideally with matrix element corrections to describe the higher jet multiplicities correctly. Both channels, electron and muon, are part of this analysis and should be run simultaneously.\end{itemize}

\noindent Cross sections, in both the electron and muon decay modes of the W boson, are presented as a function of jet multiplicity and of the transverse momentum of the leading and next-to-leading jets in the event. Measurements are also presented of the ratio of cross sections for inclusive jet multiplicities. The results, based on an integrated luminosity of 1.3 pb-1, have been corrected for all known detector effects and are quoted in a limited and well-defined range of jet and lepton kinematics.

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\typeout{Handling analysis ATLAS_2011_I894867}\subsection[ATLAS\_2011\_I894867]{ATLAS\_2011\_I894867\,\cite{Aad:2011eu}}
\textbf{Measurement of the inelastic proton-proton cross-section at sqrt{s}=7 TeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Anton Karneyeu $\langle\,$\href{mailto:Anton.Karneyeu@cern.ch}{Anton.Karneyeu@cern.ch}$\,\rangle$
  \item Sercan Sen $\langle\,$\href{mailto:Sercan.Sen@cern.ch}{Sercan.Sen@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1104.0326}{1104.0326}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inelastic events (non-diffractive and inelastic diffractive).\end{itemize}

\noindent Inelastic cross-section is measured for $\xi > 5 \times 10^{-6}$, where $\xi=M_X^2/s$ is calculated from the invariant mass, $M_X$, of hadrons selected using the largest rapidity gap in the event.

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\typeout{Handling analysis ATLAS_2011_I919017}\subsection[ATLAS\_2011\_I919017]{ATLAS\_2011\_I919017\,\cite{Aad:2011gn}}
\textbf{Measurement of ATLAS track jet properties at 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Seth Zenz $\langle\,$\href{mailto:seth.zenz@cern.ch}{seth.zenz@cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D 84 (2011) 054001
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.84.054001}{10.1103/PhysRevD.84.054001}
  \item arXiv: \href{http://arxiv.org/abs/1107.3311}{1107.3311}
  \item ATLAS-STDM-2010-14
  \item CERN-PH-EP-2011-110
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Min bias QCD at 7 TeV.\end{itemize}

\noindent ATLAS measurement of track jet \pT, multiplicity per jet, longitudinal fragmentation, transverse momentum, radius w.r.t jet axis distributions, with jets constructed from charged tracks with $\pT > 300$ MeV, using the anti-$k_T$ jet algorithm with $R = 0.4, 0.6$.

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\typeout{Handling analysis ATLAS_2011_I925932}\subsection[ATLAS\_2011\_I925932]{ATLAS\_2011\_I925932\,\cite{Aad:2011fp}}
\textbf{Measurement of the W \pT with electrons and muons at 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Elena Yatsenko $\langle\,$\href{mailto:elena.yatsenko@desy.de}{elena.yatsenko@desy.de}$\,\rangle$
  \item Judith Katzy $\langle\,$\href{mailto:jkatzy@mail.cern.ch}{jkatzy@mail.cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1108.6308v1}{1108.6308v1}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Run with $W$ decays to $e\,\nu_e$ and/or $\mu\,\nu_\mu$.\end{itemize}

\noindent The W \pT at $\sqrt{s} = 7$\;TeV is measured using $W\to e \, \nu_e$ and $W\to \mu \, \nu_\mu$ decay channels. The dressed leptons kinematics calculated from the sum of the post-FSR lepton momentum and the momenta of all photons radiated in a cone around the lepton, while the bare uses the lepton kinematics after all QED radiation.

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\typeout{Handling analysis ATLAS_2011_I926145}\subsection[ATLAS\_2011\_I926145]{ATLAS\_2011\_I926145\,\cite{Aad:2011rr}}
\textbf{Measurement of electron and muon differential cross-section from heavy-flavour decays}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9185208}{9185208}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Paul Bell $\langle\,$\href{mailto:paul.bell@cern.ch}{paul.bell@cern.ch}$\,\rangle$
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CERN-PH-EP-2011-108
  \item arXiv: \href{http://arxiv.org/abs/1109.0525}{1109.0525}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp to ele + X or mu + X at 7 TeV, heavy-flavour (bb and cc) production with B/D \ensuremath{\to} ele or muon\end{itemize}

\noindent Measurement of inclusive electron and muon cross sections for $7 < \\pT <26$~GeV in  $|\eta| <2.0$, excluding $1.37<|\eta|<1.52$, and muon cross section for $4 < \\pT < 100$~GeV in  $|\eta| <2.50$. W/Z/gamma* component must be subtracted to leave the heavy flavour contribution.

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\typeout{Handling analysis ATLAS_2011_I944826}\subsection[ATLAS\_2011\_I944826]{ATLAS\_2011\_I944826\,\cite{Aad:2011hd}}
\textbf{KS0 and Lambda production at 0.9 and 7 TeV with ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1111.1297v2}{1111.1297v2}
  \item Phys.Rev. D85 (2012) 012001
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events, 900GeV and 7TeV, Lambdas and Kshorts must be able to decay. Allow only charged decay modes to improve efficiency.\end{itemize}

\noindent The production of Kshort and Lambda hadrons is studied in inelastic pp collisions at \ensuremath{\sqrt{s}} = 0.9 and 7 TeV collected with the ATLAS detector at the LHC using a minimum-bias trigger. The observed distributions of transverse momentum, rapidity, and multiplicity are corrected to hadron level in a model-independent way within well defined phase-space regions. The distribution of the production ratio of Lambdabar to Lambda baryons is also measured. The results are compared with various Monte Carlo simulation models. Although most of these models agree with data to within 15% in the Kshort distributions, substantial disagreements with data are found in the Lambda distributions of transverse momentum. 

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\typeout{Handling analysis ATLAS_2011_I945498}\subsection[ATLAS\_2011\_I945498]{ATLAS\_2011\_I945498\,\cite{Aad:2011qv}}
\textbf{Z+jets in pp at 7TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} UNVALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Evelin Meoni evelin.meoni@cern.ch
  \item Holger Schulz
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1111.2690v1}{1111.2690v1}
  \item CERN-PH-EP-2011-162
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Z+jets, electronic and muonic Z-decays. Jets with transverse momentum $p_T > 30$ GeV and jet rapidity $|y| < 4.4$.\end{itemize}

\noindent Production of jets in association with a $Z/\gamma^*$ boson in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector. The analysis includes the full 2010 data set, collected with a low rate of multiple proton-proton collisions in the accelerator, corresponding to an integrated luminosity of 36 pb$^{-1}$. Inclusive jet cross sections in $Z/\gamma^*$ events, with $Z/\gamma^*$ decaying into electron or muon pairs, are measured for jets with transverse momentum $p_T > 30$ GeV and jet rapidity $|y| < 4.4$.

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\clearpage

\typeout{Handling analysis ATLAS_2011_I954993}\subsection[ATLAS\_2011\_I954993]{ATLAS\_2011\_I954993\,\cite{Aad:2011cx}}
\textbf{WZ fiducial cross-section at 7 TeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lynn Marx $\langle\,$\href{mailto:Lynn.Marx@hep.manchester.ac.uk}{Lynn.Marx@hep.manchester.ac.uk}$\,\rangle$
  \item Roman Lysak $\langle\,$\href{mailto:lysak@fzu.cz}{lysak@fzu.cz}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett. B709 (2012) 341-357
  \item arXiv: \href{http://arxiv.org/abs/1111.5570}{1111.5570}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp WZ events at 7 TeV  with direct e, mu W/Z boson decays (no taus from W/Z)\end{itemize}

\noindent This is a measurement of WZ production in 1.02 $fb^{-1}$ of pp collision data at $\sqrt{s} = $7 TeV collected by the ATLAS experiment in 2011. Doubly leptonic decay events are selected with electrons, muons and missing transverse momentum in the final state. The measurement of the combined fiducial cross section for the WZ bosons decaying directly into electrons and muons is performed.

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\typeout{Handling analysis ATLAS_2011_S8924791}\subsection{ATLAS\_2011\_S8924791}
\textbf{Jet shapes at 7 TeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8924791}{8924791}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Francesc Vives $\langle\,$\href{mailto:fvives@ifae.es}{fvives@ifae.es}$\,\rangle$
  \item Judith Katzy $\langle\,$\href{mailto:judith.katzy@cern.ch}{judith.katzy@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1101.0070}{1101.0070}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 7TeV GeV, corresponding to JX samples. Matching plots to kinematic \pT cut samples, or merging from slices or \pT-enhanced sampling is advised.\end{itemize}

\noindent Measurement of jet shapes in inclusive jet production in pp collisions at 7 TeV based on 3pb$^-1$ of data. Jets are reconstructed in $|\eta| < 5$ using the anti-$k_\perp$ algorithm with $30 < \pT < 600$ GeV and $|y| < 2.8$.

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\clearpage

\typeout{Handling analysis ATLAS_2011_S8971293}\subsection[ATLAS\_2011\_S8971293]{ATLAS\_2011\_S8971293\,\cite{Aad:2011ni}}
\textbf{Dijet azimuthal decorrelations}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8971293}{8971293}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1102.2696}{1102.2696}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 7000 GeV. The distributions are binned in leading \pT starting at 110 GeV with the last bin starting at 800 GeV.\end{itemize}

\noindent Dijet azimuthal decorrelation measured by ATLAS at 7 TeV. Jets are anti- kt with $R=0.6$, $p_\perp>100$ GeV, $|\eta|<0.8$. The analysis is binned in  leading jet $p_\perp$ bins. All data is fully corrected.

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\clearpage

\typeout{Handling analysis ATLAS_2011_S8983313}\subsection[ATLAS\_2011\_S8983313]{ATLAS\_2011\_S8983313\,\cite{daCosta:2011qk}}
\textbf{0-lepton squark and gluino search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8983313}{8983313}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item David Grellscheid $\langle\,$\href{mailto:david.grellscheid@durham.ac.uk}{david.grellscheid@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1102.5290}{1102.5290}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent 0-lepton search for squarks and gluinos by ATLAS at 7 TeV with an integrated luminosity of $35\,\mathrm{pb}^{-1}$. Event counts in four signal regions A-D are implemented as one-bin histograms.

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\typeout{Handling analysis ATLAS_2011_S8994773}\subsection{ATLAS\_2011\_S8994773}
\textbf{Calo-based underlying event at 900 GeV and 7 TeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8994773}{8994773}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Jinlong Zhang $\langle\,$\href{mailto:jinlong@mail.cern.ch}{jinlong@mail.cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1103.1816}{1103.1816}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 900 GeV and 7 TeV. Diffractive events should be included, but only influence the lowest bins. Multiple kinematic cuts should not be required.\end{itemize}

\noindent Underlying event measurements with the ATLAS detector at the LHC at center-of-mass energies of 900 GeV and 7 TeV, using calorimeter clusters rather than charged tracks.

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\typeout{Handling analysis ATLAS_2011_S9002537}\subsection{ATLAS\_2011\_S9002537}
\textbf{Muon charge asymmetry in W events at 7 TeV in ATLAS}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9002537}{9002537}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Krauss $\langle\,$\href{mailto:frank.krauss@durham.ac.uk}{frank.krauss@durham.ac.uk}$\,\rangle$
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1103.2929}{1103.2929}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item W \ensuremath{\to} munu events at 7 TeV\end{itemize}

\noindent Measurement of the muon charge asymmetry from W bosons produced in proton-proton collisions at a centre-of-mass energy of 7 TeV with ATLAS. The asymmetry is measured in the $W \rightarrow \mu$ decay mode as a function of the muon pseudorapidity using a data sample corresponding to a total integrated luminosity of 31pb$^-1$.

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\clearpage

\typeout{Handling analysis ATLAS_2011_S9019561}\subsection[ATLAS\_2011\_S9019561]{ATLAS\_2011\_S9019561\,\cite{Aad:2011xm}}
\textbf{Two lepton supersymmetry search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9019561}{9019561}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Angela Chen $\langle\,$\href{mailto:aqchen@fas.harvard.edu}{aqchen@fas.harvard.edu}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1103.6214}{1103.6214}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent 2-lepton search for supersymmetric particles by ATLAS at 7 TeV. Event counts in signal regions (3 same sign and 3 opposite sign) are implemented as one bin histograms. Histograms for missing transverse energy are implemented.

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\typeout{Handling analysis ATLAS_2011_S9120807}\subsection{ATLAS\_2011\_S9120807}
\textbf{Inclusive isolated diphoton analysis}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9120807}{9120807}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Giovanni Marchiori $\langle\,$\href{mailto:giovanni.marchiori@cern.ch}{giovanni.marchiori@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1107.0581}{1107.0581}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive diphoton+X events at $\sqrt{s} = 7$~TeV.\end{itemize}

\noindent A measurement of the cross section for inclusive isolated photon production at $sqrt{s} = 7$ TeV. The measurement is done in bins of $M_{\gamma\gamma}$, $p_{T\gamma\gamma}$, and $\Delta\phi_{\gamma\gamma}$, for isolated photons with $|\eta|<2.37$ and $E_T^\gamma>16$~GeV. The measurement uses 37 pb$^{-1}$ of integrated luminosity collected with the ATLAS detector.

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\clearpage

\typeout{Handling analysis ATLAS_2011_S9126244}\subsection{ATLAS\_2011\_S9126244}
\textbf{Measurement of dijet production with a veto on additional central jet activity}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9126244}{9126244}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Graham Jones $\langle\,$\href{mailto:grahamj@cern.ch}{grahamj@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1107.1641}{1107.1641}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Require QCD interactions at 7TeV. A substantial number of events are required to populate the large rapidity seperation region.\end{itemize}

\noindent A measurement of the jet activity in rapidity intervals bounded by a dijet system. The fraction of events passing a veto requirement are shown as a function of both the rapidity interval size and the average transverse momentum of the dijet system. The average number of jets above the veto threshold are also shown as a function of the same variables. There are two possible selection criteria applied to data. Either the two highest transverse momentum jets or the jets most forward and backward in rapidity are taken to define the dijet system, where the veto threhsold is 20GeV. Additionally for the latter selection an alternative veto transverse momentum threshold which is equal to the average transverse momentum is applied. Jet selections are based on anti-kt with $R=0.6$, $p_\perp>20$ GeV and $|y|<4.4$.

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\typeout{Handling analysis ATLAS_2011_S9128077}\subsection[ATLAS\_2011\_S9128077]{ATLAS\_2011\_S9128077\,\cite{Collaboration:2011tq}}
\textbf{Measurement of multi-jet cross sections}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9128077}{9128077}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1107.2092}{1107.2092}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Pure QCD, inclusive enough for jet \pT down to 60 GeV.\end{itemize}

\noindent Inclusive multi-jet production is studied using an integrated luminosity of 2.4 pb-1. Results on multi-jet cross sections are presented differential in \pT of the four leading jets, HT. Additionally three-to-two jet fractions are presented differential in different observables. Jets are anti-kt with $R=0.4$ and $R=0.6$, $p_\perp>80(60)$ GeV and $|\eta|<2.8$.

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\typeout{Handling analysis ATLAS_2011_S9131140}\subsection[ATLAS\_2011\_S9131140]{ATLAS\_2011\_S9131140\,\cite{Aad:2011gj}}
\textbf{Measurement of the Z \pT with electrons and muons at 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9131140}{9131140}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Elena Yatsenko $\langle\,$\href{mailto:elena.yatsenko@desy.de}{elena.yatsenko@desy.de}$\,\rangle$
  \item Judith Katzy $\langle\,$\href{mailto:jkatzy@mail.cern.ch}{jkatzy@mail.cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1107.2381}{1107.2381}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Run with inclusive $Z$ events, with $Z/\gamma^*$ decays to electrons and/or muons.\end{itemize}

\noindent The Z \pT at $\sqrt{s} = 7$\;TeV is measured using electron and muon $Z$ decay channels. The dressed leptons definition uses photons clustered in a cone around the charged leptons, while the bare lepton definition uses the post-FSR charged leptons only in the $Z$ reconstruction. The data used in the bare leptons calculation are based on a forward application of a PHOTOS-based energy loss correction and are hence not quite model-independent.

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\typeout{Handling analysis ATLAS_2011_S9212183}\subsection[ATLAS\_2011\_S9212183]{ATLAS\_2011\_S9212183\,\cite{Aad:2011ib}}
\textbf{0-lepton squark and gluino search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9212183}{9212183}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Chris Wymant $\langle\,$\href{mailto:c.m.wymant@durham.ac.uk}{c.m.wymant@durham.ac.uk}$\,\rangle$
  \item David Grellscheid $\langle\,$\href{mailto:david.grellscheid@durham.ac.uk}{david.grellscheid@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1109.6572}{1109.6572}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent 0-lepton search for squarks and gluinos by ATLAS at 7 TeV with an integrated luminosity of $1.04\,\mathrm{fb}^{-1}$. Event counts in five signal regions are implemented as one-bin histograms.

\clearpage


\clearpage

\typeout{Handling analysis ATLAS_2011_S9225137}\subsection[ATLAS\_2011\_S9225137]{ATLAS\_2011\_S9225137\,\cite{Aad:2011qa}}
\textbf{High jet multiplicity squark and gluino search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9225137}{9225137}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:peter.richardson@durham.ac.uk}{peter.richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1110.2299}{1110.2299}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent Search for SUSY using events with 6 or more jets in association with missing transverse momentum produced in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample has a total integrated luminosity of 1.34 fb$^{-1}$. Distributions in the W and top control regions are not produced, while in addition to the plots from the paper the count of events in the different signal regions is included.

\clearpage


\clearpage

\typeout{Handling analysis ATLAS_2012_CONF_2012_001}\subsection{ATLAS\_2012\_CONF\_2012\_001}
\textbf{4 or more lepton plus missing transverse energy SUSY search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} PRELIMINARY\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:peter.richardson@durham.ac.uk}{peter.richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item ATLAS-CONF-2012-001
  \item ATLAS-CONF-2012-035
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent Search for SUSY using events with 4 or more leptons in association with missing transverse energy in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample has a total integrated luminosity of 2.06 fb$^{-1}$. There is no reference data and in addition to the control plots from the paper the number of events in the two signal regions, correctly normalized to an integrated luminosity 2.06 fb$^{-1}$, are calculated.

\clearpage


\clearpage

\typeout{Handling analysis ATLAS_2012_I1082936}\subsection[ATLAS\_2012\_I1082936]{ATLAS\_2012\_I1082936\,\cite{Aad:2011fc}}
\textbf{Inclusive jet and dijet cross sections at 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz hschulz@physik.hu-berlin.de
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1112.6297v2}{1112.6297v2}
  \item CERN-PH-EP-2011-192
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD jet production with a minimum leading jet \pT of 30 GeV and minimum second jet \pT of 20 GeV at 7 TeV.\end{itemize}

\noindent Inclusive jet and dijet cross sections have been measured in proton-proton collisions at a centre-of-mass energy of 7 TeV using the ATLAS detector at the Large Hadron Collider. The cross sections were measured using jets clustered with the anti-kT algorithm with parameters R=0.4 and R=0.6. These measurements are based on the 2010 data sample, consisting of a total integrated luminosity of 37 inverse picobarns. Inclusive jet double-differential cross sections are presented as a function of jet transverse momentum, in bins of jet rapidity. Dijet double-differential cross sections are studied as a function of the dijet invariant mass, in bins of half the rapidity separation of the two leading jets. The measurements are performed in the jet rapidity range $|y|<4.4$, covering jet transverse momenta from 20 GeV to 1.5 TeV and dijet invariant masses from 70 GeV to 5 TeV. This is the successor analysis of ATLAS_2010_S8817804

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\typeout{Handling analysis ATLAS_2012_I1084540}\subsection{ATLAS\_2012\_I1084540}
\textbf{Rapidity gap cross sections measured with the ATLAS detector in pp collisions at \ensuremath{\sqrt{s}} = 7 TeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1084540}{1084540}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Oldrich Kepka $\langle\,$\href{mailto:kepkao@fzu.cz}{kepkao@fzu.cz}$\,\rangle$
  \item Tim Martin $\langle\,$\href{mailto:tim.martin@cern.ch}{tim.martin@cern.ch}$\,\rangle$
  \item Paul Newman $\langle\,$\href{mailto:Paul.Newman@cern.ch}{Paul.Newman@cern.ch}$\,\rangle$
  \item Pavel Ruzicka $\langle\,$\href{mailto:ruzicka@fzu.cz}{ruzicka@fzu.cz}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1201.2808}{1201.2808}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Minimum bias inelastic pp collision at 7 TeV including diffractive component and overall cross section.\end{itemize}

\noindent Pseudorapidity gap distributions in proton-proton collisions at \ensuremath{\sqrt{s}} = 7 TeV are studied using a minimum bias data sample with an integrated luminosity of 7.1 inverse microbarns. Cross sections are measured differentially in terms of Delta eta F, the larger of the pseudorapidity regions extending to the limits of the ATLAS sensitivity, at eta = +/- 4.9, in which no final state particles are produced above a transverse momentum threshold p_T Cut. The measurements span the region 0 < Delta eta F < 8 for 200 < p_T Cut < 800 MeV. At small Delta eta F, the data test the reliability of hadronisation models in describing rapidity and transverse momentum fluctuations in final state particle production. The measurements at larger gap sizes are dominated by contributions from the single diffractive dissociation process (pp \ensuremath{\to} Xp), enhanced by double dissociation (pp \ensuremath{\to} XY) where the invariant mass of the lighter of the two dissociation systems satisfies M_Y <~ 7 GeV. The resulting cross section is d sigma / d Delta eta F ~ 1 mb for Delta eta F >~ 3. The large rapidity gap data are used to constrain the value of the pomeron intercept appropriate to triple Regge models of soft diffraction. The cross section integrated over all gap sizes is compared with other LHC inelastic cross section measurements. 

\clearpage


\clearpage

\typeout{Handling analysis ATLAS_2012_I1091481}\subsection[ATLAS\_2012\_I1091481]{ATLAS\_2012\_I1091481\,\cite{:2012fa}}
\textbf{Azimuthal ordering of charged hadrons}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} UNVALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Sharka Todorova $\langle\,$\href{mailto:sarka.todorova@cern.ch}{sarka.todorova@cern.ch}$\,\rangle$
  \item Holger Schulz $\langle\,$\href{mailto:hschulz@physik.hu-berlin.de}{hschulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CERN-PH-EP-2011-197
  \item arXiv: \href{http://arxiv.org/abs/1203.0419}{1203.0419}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events with diffractives switched on.\end{itemize}

\noindent Measurement of the ordering of charged hadrons in the azimuthal angle relative to the beam axis at the Large Hadron Collider (LHC). A spectral analysis of correlations between longitudinal and transverse components of the momentum of the charged hadrons is performed. Data were recorded with the ATLAS detector at centre-of-mass energies of $\sqrt{s} = \unit{900}{\GeV}$ and $\sqrt{s} = \unit{7}{\TeV}$. The correlations measured in a phase space region dominated by low-\pT particles are not well described by conventional models of hadron production. The measured spectra show features consistent with the fragmentation of a QCD string represented by a helix-like ordered gluon chain.

\clearpage


\clearpage

\typeout{Handling analysis ATLAS_2012_I1093738}\subsection[ATLAS\_2012\_I1093738]{ATLAS\_2012\_I1093738\,\cite{Aad:2012cv}}
\textbf{Isolated prompt photon + jet xsection}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1093738}{1093738}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Giovanni Marchiori $\langle\,$\href{mailto:giovanni.marchiori@cern.ch}{giovanni.marchiori@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1203.3161}{1203.3161}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive photon+jet+X events at $\sqrt{s} = 7$~TeV.\end{itemize}

\noindent A measurement of the production cross section for isolated photons in association with jets in $pp$ collisions at $sqrt{s} = 7$ TeV. Photons with $|\eta|<1.37$ and $E_T>25$~GeV and jets with $|y|<4.4$ and $p_T>20$ GeV are selected. The differential cross section as a function of the photon transverse energy is measured, for three leading jet rapidity configurations, separately for the cases where the photon and jet rapidities have the same or the opposite sign. The measurement uses 37 pb$^{-1}$ of integrated luminosity collected with the ATLAS detector.

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\clearpage

\typeout{Handling analysis ATLAS_2012_I1094061}\subsection[ATLAS\_2012\_I1094061]{ATLAS\_2012\_I1094061\,\cite{ATLAS:2012ap}}
\textbf{Measurement of two-particle correlation function at 900 GeV and 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item James Monk $\langle\,$\href{mailto:jmonk@cern.ch}{jmonk@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item JHEP 1205 (2012) 157
  \item CERN-PH-EP-2012-011
  \item DOI: \href{http://dx.doi.org/10.1007/JHEP05(2012)157}{10.1007/JHEP05(2012)157}
  \item arxiv:1203.3549
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Soft-QCD proton-proton interactions (including diffraction) at 900 GeV or 7 TeV. Generated events should include an average lifetime cut of ctau < 10mm\end{itemize}

\noindent Two-particle angular correlations are measured in proton-proton collisions at $\\ensuremath{\sqrt{s}}=900$ GeV and 7 TeV.  Correlations are determined for charged particles with $\\pT > 100 MeV$ and $|\eta| < 2.5$.  A complicated function of both pseudorapidity and azimuth is observed.  Results are obtained from an inclusive sample of events (900 GeV and 7 TeV), as well as a sample satisfying $n_{ch} \ge 20$ (7 TeV only).

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\clearpage

\typeout{Handling analysis ATLAS_2012_I1094568}\subsection{ATLAS\_2012\_I1094568}
\textbf{Measurement of ttbar production with a veto on additional central jet activity}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1094568}{1094568}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Kiran Joshi $\langle\,$\href{mailto:kiran.joshi@cern.ch}{kiran.joshi@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1203.5015}{1203.5015}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Require dileptonic ttbar events at 7TeV.\end{itemize}

\noindent A measurement of the additional jet activity in dileptonic ttbar events. The fraction of events passing a veto requirement are shown as a function the veto scale for four central rapidity intervals. Two veto definitions are used: events are vetoed if they contain an additional jet in the rapidity interval with transverse momentum above a threshold, or alternatively, if the scalar transverse momentum sum of all additional jets in the rapidity interval is above a threshold.

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\clearpage

\typeout{Handling analysis ATLAS_2012_I1112263}\subsection[ATLAS\_2012\_I1112263]{ATLAS\_2012\_I1112263\,\cite{Aad:2012I1112263}}
\textbf{3 lepton plus missing transverse energy SUSY search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:peter.richardson@durham.ac.uk}{peter.richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item ATLAS-CONF-2012-023
  \item arXiv: \href{http://arxiv.org/abs/1204.5638}{1204.5638}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent Search for SUSY using events with 3 leptons in association with missing transverse energy in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample has a total integrated luminosity of 2.06 fb$^{-1}$. There is no reference data and in addition to the control plots from the paper the number of events in the two signal regions, correctly normalized to an integrated luminosity 2.06 fb$^{-1}$, are calculated.

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\clearpage

\typeout{Handling analysis ATLAS_2012_I1117704}\subsection{ATLAS\_2012\_I1117704}
\textbf{High jet multiplicity squark and gluino search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:peter.richardson@durham.ac.uk}{peter.richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1206.1760}{1206.1760}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent Search for SUSY using events with 6 or more jets in association with missing transverse momentum produced in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample has a total integrated luminosity of 4.7 fb$^{-1}$. Distributions in the W and top control regions are not produced, while in addition to the plots from the paper the count of events in the different signal regions is included.

\clearpage


\clearpage

\typeout{Handling analysis ATLAS_2012_I1118269}\subsection[ATLAS\_2012\_I1118269]{ATLAS\_2012\_I1118269\,\cite{:2012fc}}
\textbf{Measurement of the b-hadron production cross section using decays to $D^{*}\mu^-X$ final states in pp collisions at \ensuremath{\sqrt{s}} = 7 TeV with the ATLAS detector}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9626190}{9626190}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@ed.ac.uk}{andy.buckley@ed.ac.uk}$\,\rangle$
  \item Sercan Sen $\langle\,$\href{mailto:sercan.sen@cern.ch}{sercan.sen@cern.ch}$\,\rangle$
  \item Peter Skands $\langle\,$\href{mailto:Peter.Skands@cern.ch}{Peter.Skands@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1206.3122}{1206.3122}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp to b-hadron + X at 7 TeV, i.e. switch on "HardQCD:gg2bbbar" and "HardQCD:qqbar2bbbar" flags in Pythia8.\end{itemize}

\noindent Measurement of $b$-hadron production cross section using 3.3 pb$^{-1}$ of integrated luminosity, collected during the 2010 LHC run. The $b$-hadrons are selected by partially reconstructing $D^{*}\mu^-X$ final states using only direct semileptonic decays of $b$ to $D^{*}\mu^-X$. Differential cross sections as functions of $p_\perp$ and $|\eta|$.

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\typeout{Handling analysis ATLAS_2012_I1119557}\subsection[ATLAS\_2012\_I1119557]{ATLAS\_2012\_I1119557\,\cite{Aad:2012meb}}
\textbf{Jet shapes and jet masses}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lily Asquith $\langle\,$\href{mailto:lasquith@hep.anl.gov}{lasquith@hep.anl.gov}$\,\rangle$
  \item Roman Lysak $\langle\,$\href{mailto:lysak@fzu.cz}{lysak@fzu.cz}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev. D86 (2012) 072006
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.86.072006}{10.1103/PhysRevD.86.072006}
  \item arXiv: \href{http://arxiv.org/abs/1206.5369}{1206.5369}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD events at 7 TeV, leading-\pT jets with $\\pT > 300\;GeV$.\end{itemize}

\noindent Measurements are presented of the properties of high transverse momentum jets, produced in proton-proton collisions at a center-of-mass energy of $\sqrt{s} = 7$\;TeV. Jet mass, width, eccentricity, planar flow and angularity are measured for jets reconstructed using the anti-$k_t$ algorithm with distance parameters $R = 0.6$ and 1.0, with transverse momentum $\pT > 300$\;GeV and pseudorapidity $|\eta| < 2$.

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\typeout{Handling analysis ATLAS_2012_I1125575}\subsection[ATLAS\_2012\_I1125575]{ATLAS\_2012\_I1125575\,\cite{:2012fs}}
\textbf{Distributions sensitive to the underlying event are studied in events containing one or more charged-particle.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Kiran Joshi $\langle\,$\href{mailto:kiran.joshi@cern.ch}{kiran.joshi@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1208.0563}{1208.0563}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Minimum bias events at 7 TeV.\end{itemize}

\noindent Distributions sensitive to the underlying event are studied in events containing one or more charged-particle. Jets are reconstructed using the antikt algorithm with radius parameter R varying between 0.2 and 1.0. Distributions of the charged-particle multiplicity, the scalar sum of the transverse momentum of charged particles, and the average charged-particle \pT are measured as functions of \pT^JET in regions transverse to and opposite the leading jet for 4 GeV < \pT^JET < 100 GeV. In addition, the R-dependence of the mean values of these observables is studied.

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\typeout{Handling analysis ATLAS_2012_I1125961}\subsection{ATLAS\_2012\_I1125961}
\textbf{0-lepton squark and gluino search}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
  \item David Grellscheid $\langle\,$\href{mailto:david.grellscheid@durham.ac.uk}{david.grellscheid@durham.ac.uk}$\,\rangle$
  \item Chris Wymant $\langle\,$\href{mailto:c.m.wymant@durham.ac.uk}{c.m.wymant@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1208.0949}{1208.0949}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent 0-lepton search for squarks and gluinos by ATLAS at 7 TeV. Event counts in five signal regions are implemented as one-bin histograms.

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\typeout{Handling analysis ATLAS_2012_I1183818}\subsection[ATLAS\_2012\_I1183818]{ATLAS\_2012\_I1183818\,\cite{:2012dr}}
\textbf{pseudorapidity dependence of the total transverse energy at 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Robindra Prabhu $\langle\,$\href{mailto:prabhu@cern.ch}{prabhu@cern.ch}$\,\rangle$
  \item Peter Wijeratne $\langle\,$\href{mailto:paw@hep.ucl.ac.uk}{paw@hep.ucl.ac.uk}$\,\rangle$
  \item Roman Lysak $\langle\,$\href{mailto:lysak@fzu.cz}{lysak@fzu.cz}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1208.6256}{1208.6256}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 7 TeV, min bias and di-jet events\end{itemize}

\noindent The measurement of the sum of the transverse energy of particles as a function of particle pseudorapidity, eta, in proton-proton collisions at a centre-of-mass energy, $\\ensuremath{\sqrt{s}} = 7 TeV$ using the ATLAS detector at the Large Hadron Collider. The measurements are performed in the region $|\eta| < 4.8$ for two event classes: those requiring the presence of particles with a low transverse momentum and those requiring particles with a significant transverse momentum (dijet events where both jets have $E_T > 20$ GeV). In the second dataset measurements are made in the region transverse to the hard scatter.

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\typeout{Handling analysis ATLAS_2012_I1188891}\subsection[ATLAS\_2012\_I1188891]{ATLAS\_2012\_I1188891\,\cite{Aad:2012ma}}
\textbf{flavour composition of dijet events at 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC 7TeV)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Cecile Lapoire $\langle\,$\href{mailto:clapoire@cern.ch}{clapoire@cern.ch}$\,\rangle$
  \item Roman Lysak $\langle\,$\href{mailto:lysak@fzu.cz}{lysak@fzu.cz}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1210.0441}{1210.0441}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp di-jet events at 7 TeV\end{itemize}

\noindent The measurement of the flavour composition of dijet events produced in pp collisions at $\sqrt{s}=7 TeV$ using the ATLAS detector. Six possible combinations of light, charm and bottom jets are identified in the dijet events, where the jet flavour is defined by the presence of bottom, charm or solely light flavour hadrons in the jet. The fractions of these dijet flavour states as functions of the leading jet transverse momentum in the range 40 GeV to 500 GeV and jet rapidity $|y| < 2.1$ are measured.

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\typeout{Handling analysis ATLAS_2012_I943401}\subsection[ATLAS\_2012\_I943401]{ATLAS\_2012\_I943401\,\cite{Aad:2011cwa}}
\textbf{Search for supersymmetry with 2 leptons and missing transverse energy}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1110.6189}{1110.6189}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item BSM signal events at 7000 GeV.\end{itemize}

\noindent Results of three searches for the production of supersymmetric particles decaying into final states with missing transverse momentum and exactly two isolated leptons, electrons or muons. The analysis uses a data sample collected during the first half of 2011 that corresponds to a total integrated luminosity of 1 $\text{fb}^{-1}$ of $\sqrt{s} = 7$\,TeV proton-proton collisions recorded with the ATLAS detector at the Large Hadron Collider. Opposite-sign and same-sign dilepton events are studied separately. Additionally, in opposite- sign events, a search is made for an excess of same-flavour over different-flavour lepton pairs.

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\typeout{Handling analysis ATLAS_2013_I1217867}\subsection[ATLAS\_2013\_I1217867]{ATLAS\_2013\_I1217867\,\cite{Aad:2013ueu}}
\textbf{kT splitting scales in W\ensuremath{\to}lv events}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} ATLAS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1302.1415}{1302.1415}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item W+jet events in the electron and/or the muon decay channel.\end{itemize}

\noindent Cluster splitting scales are measured in events containing W bosons decaying to electrons or muons. The measurement comprises the four hardest splitting scales in a kT cluster sequence of the hadronic activity accompanying the W boson, and ratios of these splitting scales.

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\typeout{Handling analysis CMS_2010_S8547297}\subsection[CMS\_2010\_S8547297]{CMS\_2010\_S8547297\,\cite{Khachatryan:2010xs}}
\textbf{Charged particle transverse momentum and pseudorapidity spectra from proton-proton collisions at 900 and 2360 GeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (1180.0, 1180.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8547297}{8547297}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item A. Knutsson
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item JHEP 02 (2010) 041
  \item DOI: \href{http://dx.doi.org/10.1007/JHEP02(2010)041}{10.1007/JHEP02(2010)041}
  \item arXiv: \href{http://arxiv.org/abs/1002.0621}{1002.0621}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Non-single-diffractive (NSD) events only. Should include double-diffractive (DD) events and non-diffractive (ND) events but NOT single-diffractive (SD) events. Examples, in Pythia6 the SD processes to be turned off are 92 and 93, and in Pythia8 the SD processes are 103 and 104 (also called SoftQCD:singleDiffractive).\end{itemize}

\noindent Charged particle spectra are measured in proton-proton collisions at center-of-mass energies 900 and 2360 GeV. The spectra are normalized to all non-single-diffractive (NSD) events using corrections for trigger and selection efficiency, acceptance, and branching ratios.  There are transverse-momentum (\pT) spectra from 0.1 to 2 GeV in bins of pseudorapidity (eta) and \pT spectra from 0.1 to 4 GeV for |eta|<2.4.  The eta spectra come from the average of three methods and cover |eta|<2.5 and are corrected to include all \pT.
The data were corrected according to the SD/DD/ND content of the CMS trigger, as predicted by pythia6. The uncertainties connected with correct or uncorrect modelling of diffraction were included in the systematic errors.

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\typeout{Handling analysis CMS_2010_S8656010}\subsection[CMS\_2010\_S8656010]{CMS\_2010\_S8656010\,\cite{Khachatryan:2010us}}
\textbf{Charged particle transverse momentum and pseudorapidity spectra from proton-proton collisions at 7000 GeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8656010}{8656010}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item A. Knutsson
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.105:022002,2010
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.105.022002}{10.1103/PhysRevLett.105.022002}
  \item arXiv: \href{http://arxiv.org/abs/1005.3299}{1005.3299}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Non-single-diffractive (NSD) events only.  Should include double-diffractive (DD) events and non-diffractive (ND) events but NOT single-diffractive (SD) events. For example, in Pythia6 the SD processes to be turned off are 92 and 93, and in Pythia8 the SD processes are 103 and 104 (also called SoftQCD:singleDiffractive).\end{itemize}

\noindent Charged particle spectra are measured in proton-proton collisions at center-of-mass energies 7000 GeV. The spectra are normalized to all non-single-diffractive (NSD) events using corrections for trigger and selection efficiency, acceptance, and branching ratios.  There are transverse-momentum (\pT) spectra from 0.1 to 2 GeV in bins of pseudorapidity (eta) and the \pT spectrum from 0.1 to 6 GeV for |eta|<2.4.  The eta spectra come from the average of three methods and cover |eta|<2.5 and are corrected to include all \pT.
The data were corrected according to the SD/DD/ND content of the CMS trigger, as predicted by pythia6. The uncertainties connected with correct or uncorrect modelling of diffraction were included in the systematic errors.

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\typeout{Handling analysis CMS_2011_I954992}\subsection[CMS\_2011\_I954992]{CMS\_2011\_I954992\,\cite{Chatrchyan:2011ci}}
\textbf{Exclusive photon-photon production of muon pairs in proton-proton collisions at $\sqrt{s} = 7$ TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9279938}{9279938}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item David d'Enterria $\langle\,$\href{mailto:dde@cern.ch}{dde@cern.ch}$\,\rangle$
  \item Jonathan Hollar $\langle\,$\href{mailto:jjhollar@mail.cern.ch}{jjhollar@mail.cern.ch}$\,\rangle$
  \item Sercan Sen $\langle\,$\href{mailto:Sercan.Sen@cern.ch}{Sercan.Sen@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1111.5536}{1111.5536}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item gamma gamma TO mu+ mu- process.\end{itemize}

\noindent A measurement of the exclusive two-photon production of muon pairs in proton-proton collisions at at a centre-of-mass energy 7 TeV with the final state $p \mu^+ \mu^- p$, is reported using data corresponding to an integrated luminosity of 40 pb$^-1$ collected in 2010.  The measured cross section is obtained with a fit to the dimuon $p_T$ distribution for muon pairs with invariant mass greater than 11.5 GeV with each muon $p_T > 4$ GeV and $|\eta| < 2.1$.

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\typeout{Handling analysis CMS_2011_S8884919}\subsection[CMS\_2011\_S8884919]{CMS\_2011\_S8884919\,\cite{Khachatryan:2010nk}}
\textbf{Measurement of the NSD charged particle multiplicity at \ensuremath{\sqrt{s}} = 0.9, 2.36, and 7 TeV with the CMS detector.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (1180.0, 1180.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8884919}{8884919}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Romain Rougny $\langle\,$\href{mailto:romain.rougny@cern.ch}{romain.rougny@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item J. High Energy Phys. 01 (2011) 079
  \item DOI: \href{http://dx.doi.org/10.1007/JHEP01(2011)079}{10.1007/JHEP01(2011)079}
  \item arXiv: \href{http://arxiv.org/abs/1011.5531}{1011.5531}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Non-single-diffractive (NSD) events only.  Should include double-diffractive (DD) events and non-diffractive (ND) events but NOT single-diffractive (SD) events. For example, in Pythia6 the SD processes to be turned off are 92 and 93 and in Pythia8 the SD processes are 103 and 104 (also called SoftQCD:singleDiffractive).\end{itemize}

\noindent Measurements of primary charged hadron multiplicity distributions are presented for non-single-diffractive events in proton-proton collisions at centre-of-mass energies of \ensuremath{\sqrt{s}} = 0.9, 2.36, and 7 TeV, in five pseudorapidity ranges from |eta|<0.5 to |eta|<2.4. The data were collected with the minimum-bias trigger of the CMS experiment during the LHC commissioning runs in 2009 and the 7 TeV run in 2010. The average transverse momentum as a function of the multiplicity is also presented. The measurement of higher-order moments of the multiplicity distribution confirms the violation of Koba-Nielsen-Olesen scaling that has been observed at lower energies.

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\typeout{Handling analysis CMS_2011_S8941262}\subsection[CMS\_2011\_S8941262]{CMS\_2011\_S8941262\,\cite{Khachatryan:2011hf}}
\textbf{Production cross-sections of muons from $b$ hadron decays in $pp$ collisions}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8941262}{8941262}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Wolfram Erdmann $\langle\,$\href{mailto:wolfram.erdmann@psi.ch}{wolfram.erdmann@psi.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item JHEP 1103,090
  \item DOI: \href{http://dx.doi.org/10.1007/JHEP03(2011)090}{10.1007/JHEP03(2011)090}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/1101.3512}{hep-ex/1101.3512}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive QCD at 7 TeV, with no \pT cuts.\end{itemize}

\noindent A measurement of the $b$-hadron production cross-section in proton-proton collisions at $\sqrt{s} = 7$~TeV. The dataset, corresponding to 85 inverse nanobarns, was recorded with the CMS experiment at the LHC using a low-threshold single-muon trigger. Events are selected by the presence of a muon with transverse momentum greater than 6 GeV with respect to the beam direction and pseudorapidity less than 2.1. The transverse momentum of the muon with respect to the closest jet discriminates events containing $b$ hadrons from background. The inclusive $b$-hadron production cross section is presented as a function of muon transverse momentum and pseudorapidity.

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\typeout{Handling analysis CMS_2011_S8950903}\subsection[CMS\_2011\_S8950903]{CMS\_2011\_S8950903\,\cite{Khachatryan:2011zj}}
\textbf{Dijet azimuthal decorrelations in $pp$ collisions at $\sqrt{s} = 7$ TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8950903}{8950903}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Tomo Umer $\langle\,$\href{mailto:tomo.umer@cern.ch}{tomo.umer@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rev. Lett. 106 (2011) 122003
  \item arXiv: \href{http://arxiv.org/abs/1101.5029}{1101.5029}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive QCD at 7TeV comEnergy, ptHat (or equivalent) greater than 20 GeV\end{itemize}

\noindent Measurements of dijet azimuthal decorrelations in pp collisions at \ensuremath{\sqrt{s}} = 7 TeV using the CMS detector at the CERN LHC are presented. The analysis is based on an inclusive dijet event sample corresponding to an integrated luminosity of 2.9/pb. Jets are anti-kt with $R=0.5$, $p_\perp>80(30)$ GeV and $|\eta|<1.1$.

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\typeout{Handling analysis CMS_2011_S8957746}\subsection[CMS\_2011\_S8957746]{CMS\_2011\_S8957746\,\cite{Khachatryan:2011dx}}
\textbf{Event shapes}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8957746}{8957746}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.B699:48-67,2011
  \item arXiv: \href{http://arxiv.org/abs/1102.0068}{1102.0068}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 7000 GeV. Particles with c*tau>10mm are stable.\end{itemize}

\noindent Central transverse Thrust and Minor have been measured in proton-proton collisions at \ensuremath{\sqrt{s}}=7 TeV, with a data sample collected with the CMS detector at the LHC. The sample corresponds to an integrated luminosity of 3.2 inverse picobarns. Input for the variables are anti-kt jets with $R=0.5$.

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\typeout{Handling analysis CMS_2011_S8968497}\subsection[CMS\_2011\_S8968497]{CMS\_2011\_S8968497\,\cite{Khachatryan:2011as}}
\textbf{Measurement of dijet angular distributions and search for quark compositeness in $pp$ collisions at $\sqrt{s} = 7$ TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (CERN LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8968497}{8968497}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item A. Hinzmann
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.106:201804,2011
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevLett.106.201804}{10.1103/PhysRevLett.106.201804}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/1102.2020}{hep-ex/1102.2020}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item ~\end{itemize}

\noindent Measurement of dijet angular distributions in proton-proton collisions at a center-of-mass energy of 7 TeV. The data sample, collected with single jet triggers, has a total integrated luminosity of 36 pb-1, with jets being reconstructed using the anti-KT clustering algorithm using R=0.5. The data are presented for the variable CHI defined as EXP(|Y1-Y2|) where Y1 and Y2 are the rapidities of the two leading (highest PT) jets.'

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\typeout{Handling analysis CMS_2011_S8973270}\subsection[CMS\_2011\_S8973270]{CMS\_2011\_S8973270\,\cite{Khachatryan:2011wq}}
\textbf{B/anti-B angular correlations based on secondary vertex reconstruction in pp collisions}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8973270}{8973270}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Lukas Wehrli $\langle\,$\href{mailto:wehrlilu@cern.ch}{wehrlilu@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item JHEP 1103 136
  \item DOI: \href{http://dx.doi.org/10.1007/JHEP03(2011)136}{10.1007/JHEP03(2011)136}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/1102.3194}{hep-ex/1102.3194}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive QCD at 7TeV comEnergy, pthat cut (or similar) recommended (leading jet pt > 56 GeV required)\end{itemize}

\noindent The differential $B\bar{B}$ cross-section is measured as a function of the opening angle $\Delta{R}$ and $\Delta\phi$ using data collected with the CMS detector during 2010 and corresponding to an integrated luminosity of 3.1 pb$^{-1}$. The measurement is performed for three different event energy scales, characterized by the transverse momentum of the leading jet in the event (above 56 GeV, above 84 GeV and above 120 GeV). Simulated events are normalised in the region $\Delta{R} > 2.4$ and $\Delta\phi > 3/4\pi$ respectively.

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\typeout{Handling analysis CMS_2011_S8978280}\subsection[CMS\_2011\_S8978280]{CMS\_2011\_S8978280\,\cite{Khachatryan:2011tm}}
\textbf{Kshort, Lambda, and Cascade- transverse momentum and rapidity spectra from proton-proton collisions at 900 and 7000 GeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8978280}{8978280}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Kevin Stenson $\langle\,$\href{mailto:kevin.stenson@colorado.edu}{kevin.stenson@colorado.edu}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item JHEP 05 (2011) 064
  \item DOI: \href{http://dx.doi.org/10.1007/JHEP05(2011)064}{10.1007/JHEP05(2011)064}
  \item arXiv: \href{http://arxiv.org/abs/1102.4282}{1102.4282}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Non-single-diffractive (NSD) events only.  Should include double-diffractive (DD) events and non-diffractive (ND) events but NOT single-diffractive (SD) events. For example, in Pythia6 the SD processes to be turned off are 92 and 93, and in Pythia8 the SD processes are 103 and 104 (also called SoftQCD:singleDiffractive).\end{itemize}

\noindent The spectra of Kshort, Lambda, and Cascade- particles were measured versus transverse-momentum (\pT) and rapidity(y) in proton-proton collisions at center-of-mass energies 900 and 7000 GeV.  The production is normalized to all non-single-diffractive (NSD) events using corrections for trigger and selection efficiency, acceptance, and branching ratios.  The results cover a rapidity range of |y|<2 and a \pT range from 0 to 10 GeV (Kshort and Lambda) and 0 to 6 GeV (Cascade-).  Antiparticles are included in all measurements so only the sum of Lambda and Lambdabar and Cascade- and anti-Cascade- are given.  The rapidity distributions are shown versus |y| but normalized to a unit of y. Ratios of Lambda/Kshort and Cascade-/Lambda production versus \pT and |y| are also given, with somewhat smaller systematic uncertainties than obtained from taking the ratio of the individual distributions.'
The data were corrected according to the SD/DD/ND content of the CMS trigger, as predicted by pythia6. The uncertainties connected with correct or uncorrect modelling of diffraction were included in the systematic errors.

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\typeout{Handling analysis CMS_2011_S9086218}\subsection[CMS\_2011\_S9086218]{CMS\_2011\_S9086218\,\cite{:2011me}}
\textbf{Measurement of the inclusive jet cross-section in $pp$ collisions at $\sqrt{s} = 7$ TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9086218}{9086218}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Rasmus Sloth Hansen<rsh07@phys.au.dk>
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item http://cdsweb.cern.ch/record/1355680
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive QCD at 7TeV comEnergy, ptHat (or equivalent) greater than 10 GeV\end{itemize}

\noindent The inclusive jet cross section is measured in pp collisions with a center-of-mass energy of 7 TeV at the LHC using the CMS experiment. The data sample corresponds to an integrated luminosity of 34 inverse picobarns. The measurement is made for jet transverse momenta in the range 18-1100 GeV and for absolute values of rapidity less than 3. Jets are anti-kt with $R=0.5$, $p_\perp>18$ GeV and $|y|<3.0$.

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\typeout{Handling analysis CMS_2011_S9088458}\subsection[CMS\_2011\_S9088458]{CMS\_2011\_S9088458\,\cite{Chatrchyan:2011wn}}
\textbf{Measurement of ratio of the 3-jet over 2-jet cross section in pp collisions at \ensuremath{\sqrt{s}} = 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9088458}{9088458}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Tomo Umer $\langle\,$\href{mailto:tomo.umer@cern.ch}{tomo.umer@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Lett. B 702 (2011) 336
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive QCD at 7TeV comEnergy, ptHat (or equivalent) greater than 30 GeV\end{itemize}

\noindent A measurement of the ratio of the inclusive 3-jet to 2-jet cross sections as a function of the total jet transverse momentum, HT, in the range 0.2 < HT < 2.5 TeV is presented. The data have been collected at a proton-proton centre-of-mass energy of 7 TeV with the CMS detector at the LHC, and correspond to an integrated luminosity of 36/pb. Jets are anti-kt with $R=0.5$, $p_\perp>50$ GeV and $|\eta|<2.5$.

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\typeout{Handling analysis CMS_2011_S9120041}\subsection[CMS\_2011\_S9120041]{CMS\_2011\_S9120041\,\cite{Chatrchyan:2011id}}
\textbf{Traditional leading jet UE measurement at $\\ensuremath{\sqrt{s}}=0.9$ and 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9120041}{9120041}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Mohammed Zakaria (mzakaria@ufl.edu)
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item J. High Energy Phys 09 (2011) 109
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Requires inclusive inelastic events (non-diffractive and inelastic diffractive). The profile plots require large statistics.\end{itemize}

\noindent A measurement of the underlying activity in scattering processes with a hard scale in the several-GeV region is performed in proton-proton collisions at Energies of 0.9 and 7 TeV, using data collected by the CMS experiment at the LHC. The production of charged particles with pseudorapidity |eta| < 2 and transverse momentum \pT > 0.5 GeV/c is studied in the azimuthal region transverse to that of the leading set of charged particles forming a track-jet. Various comparisons are made between the two different energies and also beteen two sets of cuts on \pT for leading track jet \pT-leading > 3 GeV and \pT-leading > 20 GeV. The activity is studied using 5 types of plots. 2 profile plots for the multiplcity of charged particles and the scalar sum of \pT. and 3 distributions for the two previous quantities as well we \pT for all the particles in the transverse region.

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\clearpage

\typeout{Handling analysis CMS_2011_S9215166}\subsection[CMS\_2011\_S9215166]{CMS\_2011\_S9215166\,\cite{Chatrchyan:2011wm}}
\textbf{Forward energy flow in MB and dijet events at 0.9 and 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+9215166}{9215166}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item S. Dooling $\langle\,$\href{mailto:samantha.dooling@cern.ch}{samantha.dooling@cern.ch}$\,\rangle$
  \item A. Knutsson $\langle\,$\href{mailto:albert.knutsson@cern.ch}{albert.knutsson@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item JHEP 1111 148
  \item DOI: \href{http://dx.doi.org/10.1007/JHEP11(2011)148}{10.1007/JHEP11(2011)148}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/1110.0211}{hep-ex/1110.0211}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $pp$ MB and QCD interactions at 0.9 and 7~TeV. No \pT-cuts.\end{itemize}

\noindent Forward energy flow measured by CMS at $\sqrt{s} = 0.9$ and 7~TeV in MB and dijet events.

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\clearpage

\typeout{Handling analysis CMS_2012_I1087342}\subsection[CMS\_2012\_I1087342]{CMS\_2012\_I1087342\,\cite{Chatrchyan:2012gwa}}
\textbf{Measurement of forward and forward+central jets at \ensuremath{\sqrt{s}} = 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1087342}{1087342}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Albert Knutsson $\langle\,$\href{mailto:albert.knutsson@cern.ch}{albert.knutsson@cern.ch}$\,\rangle$
  \item Rasmus Sloth Hansen $\langle\,$\href{mailto:rsh07@phys.au.dk}{rsh07@phys.au.dk}$\,\rangle$
  \item Bo Zhu
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item JHEP 1206 (2012) 036
  \item CMS-FWD-11-002
  \item CERN-PH-EP-2011-179
  \item doi 10.1007/JHEP06(2012)036
  \item arXiv: \href{http://arxiv.org/abs/1202.0704}{1202.0704}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 7 TeV.\end{itemize}

\noindent Inclusive forward jets and forward+central jets measured by CMS at \ensuremath{\sqrt{s}}=7 TeV.

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\clearpage

\typeout{Handling analysis CMS_2012_I1102908}\subsection[CMS\_2012\_I1102908]{CMS\_2012\_I1102908\,\cite{Chatrchyan:2012pb}}
\textbf{Measurement of inclusive and exclusive dijet production ratio at large rapidity intervals at center-of-mass energy 7 TeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Grzegorz Brona
  \item Vladimir Gavrilov
  \item Hannes Jung
  \item Victor Kim
  \item Victor Murzin
  \item Vadim Oreshkin
  \item Grigory Pivovarov
  \item Ivan Pozdnyakov
  \item Grigory Safronov
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CMS-FWD-10-014
  \item CERN-PH-EP-2012-088
  \item arXiv: \href{http://arxiv.org/abs/1204.0696}{1204.0696}
  \item Submitted to the EPJ C
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inclusive QCD at 7TeV comEnergy, ptHat (or equivalent) greater than 15 GeV\end{itemize}

\noindent This is a measurement of the ratio of inclusive to exclusive dijet production as a function of the absolute distance in rapidity, $\Delta y$, between jets. The ratio of the Mueller-Navelet to exclusive dijet production is also measured.  These measurements were performed with the CMS detector in proton-proton collisions at $\sqrt s = 7$ TeV for jets with $p_T > 35$ GeV and $|y| < 4.7$ taken from a mixture of two data samples, one of which containing dijets with moderate rapidity separation and the other containing dijets with large rapidity separation, with integrated luminosity of 33/nb and 5/pb respectively. The measured observables are corrected for detector effects.

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\typeout{Handling analysis CMS_2012_I1107658}\subsection[CMS\_2012\_I1107658]{CMS\_2012\_I1107658\,\cite{Chatrchyan:2012tb}}
\textbf{Measurement of the underlying event activity in the Drell-Yan process at a centre-of-mass energy of 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Sunil Bansal (sunil.bansal@cern.ch)
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CMS-QCD-11-012
  \item CERN-PH-EP-2012-085
  \item arXiv: \href{http://arxiv.org/abs/1204.1411}{1204.1411}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Drell-Yan events with $Z/\gamma^* \to \mu\mu$. $m(\mu,\mu) > 20$ GeV\end{itemize}

\noindent A measurement of the underlying event activity using Drell-Yan events using muonic final state.  The production of charged particles with pseudorapidity $|\eta| < 2$ and transverse momentum $p_\perp > 0.5\,\GeV/c$ is studied in towards, transverse and away region w.r.t. to the direction of di-muon system. The UE activity is measured in terms of of a particle density and an energy density. The particle density is computed as the average number of primary charged particles per unit pseudorapidity and per unit azimuth. The energy density is expressed in terms of the average of the scalar sum of the transverse momenta of primary charged particles per unit pseudorapidity and azimuth.  The ratio of the energy and particle density is also reported in 3 regions.  UE activity  is studied as a function of invariant mass of muon pair ($M_{\mu\mu}$) by limiting the ISR contribution by requiring transverse momentum of muon pair $p_\perp(\mu\mu) < 5\,\GeV/c$. The $p_\perp(\mu\mu)$ dependence is studied for the events having $M_{\mu\mu}$ in window of 81--101 GeV/$c$. The normalized charged particle multiplicity and $p_\perp$ spectrum of the charged particles in three regions also been reported for events having $M_{\mu\mu}$ in window of 81--101 GeV/$c$. Multiplicity and $p_\perp$ spectra in the transverse region are also reported, for events having $p_\perp(\mu\mu) < 5\,\GeV/c$.

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\typeout{Handling analysis CMS_2012_I1184941}\subsection[CMS\_2012\_I1184941]{CMS\_2012\_I1184941\,\cite{:2012vc}}
\textbf{Measurement of the differential cross section for inclusive dijet production as a function of $\xi$ in 7 TeV proton-proton collisions.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Sercan Sen $\langle\,$\href{mailto:ssen@cern.ch}{ssen@cern.ch}$\,\rangle$
  \item Alexander Proskuryakov $\langle\,$\href{mailto:aproskur@mail.cern.ch}{aproskur@mail.cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1209.1805}{1209.1805}
  \item Submitted to Phys. Rev. D
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item High statistics is needed to observe events in the lowest (xi) bin. Distributions are presented for HardQCD events (i.e., in PYTHIA with ptHatMin=15GeV) and Diffractive events.\end{itemize}

\noindent Measurement of the differential cross section for inclusive dijet production as a function of $\xi$ which approximates the fractional momentum loss of the scattered proton in single-diffraction events. The data used has a total integrated luminosity of 2.7 nb-1 collected during 2010 with low instantaneous luminosity. Events are selected with at least two jets in $|\eta| < 4.4$ with $\pT > 20$ GeV and all final states particles are used for the reconstruction of $\xi$.

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\typeout{Handling analysis CMS_2012_I1193338}\subsection[CMS\_2012\_I1193338]{CMS\_2012\_I1193338\,\cite{:2012}}
\textbf{Measurement of the inelastic proton-proton cross section at \ensuremath{\sqrt{s}}=7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Sercan Sen $\langle\,$\href{mailto:ssen@cern.ch}{ssen@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1210.6718}{1210.6718}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inelastic events (non-diffractive and inelastic diffractive).\end{itemize}

\noindent The inelastic cross-section is measured through two independent methods based on information from (i) forward calorimetry (for pseudorapidity $3 < |\eta| < 5$), in collisions where at least one proton loses more than $\xi > 5 \cdot 10^{-6}$ of its longitudinal momentum, and (ii) the central tracker ($|\eta| < 2.4$), in collisions containing an interaction vertex with more than 1, 2, or 3 tracks with $p_\perp > 200$ MeV/c.

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\clearpage

\typeout{Handling analysis CMS_2012_PAS_FWD_11_003}\subsection{CMS\_2012\_PAS\_FWD\_11\_003}
\textbf{Study of the Underlying Event at Forward Rapidity in Proton-Proton Collisions at the LHC}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (1380.0, 1380.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+~}{~}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Samantha Dooling $\langle\,$\href{mailto:samantha.dooling@desy.de}{samantha.dooling@desy.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CMS-PAS-FWD-11-003
  \item http://cdsweb.cern.ch/record/1434458
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inelastic events (non-diffractive and diffractive) at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV.\end{itemize}

\noindent Ratio of the energy deposited in the  pseudorapidity range $-6.6 < \eta < -5.2$ for events with a charged particle jet with $|\eta|<2$ with respect to the energy in  inclusive events, as a function of charged particle jet transverse momentum for $\sqrt{s}=$0.9, 2.76 and 7 TeV.

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\typeout{Handling analysis CMS_2012_PAS_QCD_11_010}\subsection[CMS\_2012\_PAS\_QCD\_11\_010]{CMS\_2012\_PAS\_QCD\_11\_010\,\cite{CMS-PAS-QCD-11-010}}
\textbf{Strange particle production in underlying events in proton--proton collisions at $\sqrt{s} = 7$ TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Status:} PRELIMINARY\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Sercan Sen $\langle\,$\href{mailto:Sercan.Sen@cern.ch}{Sercan.Sen@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CMS-PAS-QCD-11-010
  \item http://cdsweb.cern.ch/record/1463352
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inelastic events (non-diffractive and inelastic diffractive) at $\sqrt{s} = 7$\;TeV.\end{itemize}

\noindent Measurements of the production of $K^0_S$, $\Lambda$ and $\bar{Lambda}$ particles in the underlying activity of events with a \pT scale ranging from 1 to 50 GeV/$c$ in $pp$ collisions at $\sqrt{s} = 7$\;TeV.

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\clearpage

\typeout{Handling analysis CMS_QCD_10_024}\subsection[CMS\_QCD\_10\_024]{CMS\_QCD\_10\_024\,\cite{CMS-PAS-QCD-10-024}}
\textbf{Pseudorapidity distributions of charged particles at \ensuremath{\sqrt{s}}=0.9 and 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (450.0, 450.0), (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} CMS (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+~}{~}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item P. Katsas $\langle\,$\href{mailto:panagiotis.katsas@cern.ch}{panagiotis.katsas@cern.ch}$\,\rangle$
  \item A. Knutsson $\langle\,$\href{mailto:albert.knutsson@cern.ch}{albert.knutsson@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CMS-PAS-QCD-10-024
  \item https://cdsweb.cern.ch/record/1341853?ln=en
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $pp$ collisions at 0.9 and 7~TeV. Minimum bias events.\end{itemize}

\noindent Pseudorapidity distributions of charged particles in $pp$ collisions at $\sqrt{s} = 0.9$ and 7~TeV with at least one central charged particle.

\clearpage


\clearpage

\typeout{Handling analysis LHCB_2010_I867355}\subsection[LHCB\_2010\_I867355]{LHCB\_2010\_I867355\,\cite{Aaij:2010gn}}
\textbf{Measurement of sigma(pp to bbar{b} X at sqrt{s}=7 TeV in the forward region}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} LHCb (LHC)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+8785570}{8785570}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@ed.ac.uk}{andy.buckley@ed.ac.uk}$\,\rangle$
  \item Sercan Sen $\langle\,$\href{mailto:sercan.sen@cern.ch}{sercan.sen@cern.ch}$\,\rangle$
  \item Peter Skands $\langle\,$\href{mailto:Peter.Skands@cern.ch}{Peter.Skands@cern.ch}$\,\rangle$
  \item Sheldon Stone $\langle\,$\href{mailto:stone@physics.syr.edu}{stone@physics.syr.edu}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1009.2731}{1009.2731}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp to b-hadron + X at 7 TeV. i.e., Swith on "HardQCD:gg2bbbar" and "HardQCD:qqbar2bbbar" flags in pythia8(v165).\end{itemize}

\noindent The average cross-section to produce b-flavoured or bbar-flavoured hadrons is measured in different pseudorapidity intervals over the entire range of \pT assuming the LEP (and Tevatron) fractions for fragmentation into b-flavoured hadrons.

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\typeout{Handling analysis LHCF_2012_I1115479}\subsection[LHCF\_2012\_I1115479]{LHCF\_2012\_I1115479\,\cite{Adriani:2012ap}}
\textbf{Measurement of forward neutral pion transverse momentum spectra for $\sqrt{s}$ = 7 TeV proton-proton collisions at LHC}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} LHCF (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Sercan Sen $\langle\,$\href{mailto:ssen@cern.ch}{ssen@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/1205.4578}{1205.4578}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Inelastic events (ND+SD+DD) at $\sqrt{s}$ = 7 TeV.\end{itemize}

\noindent The inclusive production rate of neutral pions has been measured by LHCf experiment during $\sqrt{s}=7$ TeV pp collision operation in early 2010. In order to ensure good event reconstruction efficiency, the range of the $\pi^0$ rapidity and $p_\perp$ are limited to $8.9 < y < 11.0$ and $p_\perp < 0.6$ GeV, respectively.

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\typeout{Handling analysis TOTEM_2012_002}\subsection[TOTEM\_2012\_002]{TOTEM\_2012\_002\,\cite{Antchev:1472948}}
\textbf{Measurement of proton-proton elastic scattering and total cross section at \ensuremath{\sqrt{s}} = 7 TeV.}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} TOTEM (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Sercan Sen $\langle\,$\href{mailto:Sercan.Sen@cern.ch}{Sercan.Sen@cern.ch}$\,\rangle$
  \item Peter Skands $\langle\,$\href{mailto:Peter.Skands@cern.ch}{Peter.Skands@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item CERN-PH-EP-2012-239
  \item http://cds.cern.ch/record/1472948
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Elastic events only.\end{itemize}

\noindent Measurement of the elastic differential cross-section in proton-proton interactions at a centre-of-mass energy $\sqrt{s}=7$ TeV at the LHC. The data, which cover the $|t|$ range 0.005--0.2 $\text{GeV}^2$, were collected using Roman Pot detectors very close to the outgoing beam in October 2011, allowing the precise extrapolation down to the optical point, $t = 0$, and hence the derivation of the elastic as well as the total cross-section via the optical theorem.

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\typeout{Handling analysis TOTEM_2012_I1115294}\subsection{TOTEM\_2012\_I1115294}
\textbf{Forward dN/deta at 7 TeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (3500.0, 3500.0) GeV \newline
\textbf{Experiment:} TOTEM (LHC)\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Europhys.Lett. 98 (2012) 31002
  \item arXiv: \href{http://arxiv.org/abs/1205.4105}{1205.4105}
  \item CERN-PH-EP-2012-106
  \item TOTEM 2012-01
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp QCD interactions at 900 GeV and 7 TeV.\end{itemize}

\noindent The TOTEM experiment has measured the charged particle pseudorapidity density $dN_\text{ch}/d\eta$ in pp collisions at $\sqrt{s} = 7$\,TeV for $5.3 < |\eta| < 6.4$ in events with at least one charged particle with transverse momentum above 40 MeV/c in this pseudorapidity range.

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\section{SPS analyses}\typeout{Handling analysis UA1_1990_S2044935}\subsection[UA1\_1990\_S2044935]{UA1\_1990\_S2044935\,\cite{Albajar:1989an}}
\textbf{UA1 multiplicities, transverse momenta and transverse energy distributions.}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (31.5, 31.5), (100.0, 100.0), (250.0, 250.0), (450.0, 450.0) GeV \newline
\textbf{Experiment:} UA1 (SPS)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2044935}{2044935}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant@durham.ac.uk}{c.l.j.j.vaillant@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Nucl.Phys.B353:261,1990
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD min bias events at sqrtS = 63, 200, 500 and 900 GeV.\end{itemize}

\noindent Particle multiplicities, transverse momenta and transverse energy distributions at the UA1 experiment, at energies of 200, 500 and 900 GeV (with one plot at 63 GeV for comparison).

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\typeout{Handling analysis UA5_1982_S875503}\subsection[UA5\_1982\_S875503]{UA5\_1982\_S875503\,\cite{Alpgard:1982zx}}
\textbf{UA5 multiplicity and pseudorapidity distributions for $pp$ and $p\bar{p}$.}\newline
\textbf{Beams:} $\bar{p}$\,$p$, $p$\,$p$ \newline
\textbf{Energies:} (26.5, 26.5) GeV \newline
\textbf{Experiment:} UA5 (SPS)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+875503}{875503}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant@durham.ac.uk}{c.l.j.j.vaillant@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Lett.112B:183,1982
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Min bias QCD events at \ensuremath{\sqrt{s}} = 53~GeV. Run with both $pp$ and $p\bar{p}$ beams.\end{itemize}

\noindent Comparisons of multiplicity and pseudorapidity distributions for $pp$ and $p\bar{p}$ collisions at 53 GeV, based on the UA5 53~GeV runs in 1982. Data confirms the lack of significant difference between the two beams.

\clearpage


\clearpage

\typeout{Handling analysis UA5_1986_S1583476}\subsection[UA5\_1986\_S1583476]{UA5\_1986\_S1583476\,\cite{Alner:1986xu}}
\textbf{Pseudorapidity distributions in $p\bar{p}$ (NSD, NSD+SD) events at \ensuremath{\sqrt{s}} = 200 and 900 GeV}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (100.0, 100.0), (450.0, 450.0) GeV \newline
\textbf{Experiment:} UA5 (CERN SPS)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1583476}{1583476}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
  \item Christophe Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant@durham.ac.uk}{c.l.j.j.vaillant@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur. Phys. J. C33, 1, 1986
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item * Single- and double-diffractive, plus non-diffractive inelastic, events.
  \item $p\bar{p}$ collider, \ensuremath{\sqrt{s}} = 200 or 900 GeV.
  \item The trigger implementation for NSD events is the same as in, e.g., the UA5_1989 analysis. No further cuts are needed.\end{itemize}

\noindent This study comprises measurements of pseudorapidity distributions measured with the UA5 detector at 200 and 900 GeV center of momentum energy. There are distributions for non-single diffractive (NSD) events and also for the combination of single- and double-diffractive events. The NSD distributions are further studied for certain ranges of the events charged multiplicity.

\clearpage


\clearpage

\typeout{Handling analysis UA5_1987_S1640666}\subsection[UA5\_1987\_S1640666]{UA5\_1987\_S1640666\,\cite{Alner:1987wb}}
\textbf{UA5 charged multiplicity measurements at 546 GeV}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (273.0, 273.0) GeV \newline
\textbf{Experiment:} UA5 (CERN SPS)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1640666}{1640666}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rept.154:247-383,1987
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item QCD and diffractive events at 546 GeV\end{itemize}

\noindent Charged particle multiplicity measurement.

\clearpage


\clearpage

\typeout{Handling analysis UA5_1988_S1867512}\subsection[UA5\_1988\_S1867512]{UA5\_1988\_S1867512\,\cite{Ansorge:1988fg}}
\textbf{Charged particle correlations in UA5 $p \\bar{p}$ NSD events at \ensuremath{\sqrt{s}} = 200, 546 and 900 GeV.}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (100.0, 100.0), (273.0, 273.0), (450.0, 450.0) GeV \newline
\textbf{Experiment:} UA5 (CERN SPS)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1867512}{1867512}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys.C37:191-213,1988
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item ppbar events. Non-single diffractive events need to be switched on. The trigger implementation is the same as in UA5_1989_S1926373. Important: Only the correlation strengths with symmetric eta bins should be used for tuning.\end{itemize}

\noindent Data on two-particle pseudorapidity and multiplicity correlations of charged particles for non single-diffractive $\bar{p}p$ collisions at c.m. energies of 200, 546 and 900 GeV. Pseudorapidity correlations interpreted in terms of a cluster model, which has been motivated by this and other experiments, require on average about two charged particles per cluster. The decay width of the clusters in pseudorapidity is approximately independent of multiplicity and of c.m. energy. The investigations of correlations in terms of pseudorapidity gaps confirm the picture of cluster production. The strength of forward-backward multiplicity correlations increases linearly with ins and depends strongly on position and size of the pseudorapidity gap separating the forward and backward interval. All our correlation studies can be understood in terms of a cluster model in which clusters contain on average about two charged particles, i.e. are of similar magnitude to earlier estimates from the ISR.

\clearpage


\clearpage

\typeout{Handling analysis UA5_1989_S1926373}\subsection[UA5\_1989\_S1926373]{UA5\_1989\_S1926373\,\cite{Ansorge:1988kn}}
\textbf{UA5 charged multiplicity measurements}\newline
\textbf{Beams:} $\bar{p}$\,$p$ \newline
\textbf{Energies:} (100.0, 100.0), (450.0, 450.0) GeV \newline
\textbf{Experiment:} UA5 (CERN SPS)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+1926373}{1926373}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
  \item Christophe L. J. Vaillant $\langle\,$\href{mailto:c.l.j.j.vaillant@durham.ac.uk}{c.l.j.j.vaillant@durham.ac.uk}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z. Phys. C - Particles and Fields 43, 357-374 (1989)
  \item DOI: \href{http://dx.doi.org/10.1007/BF01506531}{10.1007/BF01506531}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Minimum bias events at \ensuremath{\sqrt{s}} = 200 and 900 GeV. Enable single and double diffractive events in addition to non-diffractive processes.\end{itemize}

\noindent Multiplicity distributions of charged particles produced in non-single-diffractive collisions between protons and antiprotons at centre-of-mass energies of 200 and 900 GeV. The data were recorded in the UA5 streamer chambers at the CERN collider, which was operated in a pulsed mode between the two energies. This analysis confirms the violation of KNO scaling in full phase space found by the UA5 group at an energy of 546 GeV, with similar measurements at 200 and 900 GeV.

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\section{HERA analyses}\typeout{Handling analysis H1_1994_S2919893}\subsection[H1\_1994\_S2919893]{H1\_1994\_S2919893\,\cite{Abt:1994ye}}
\textbf{H1 energy flow and charged particle spectra in DIS}\newline
\textbf{Beams:} $p$\,$e^-$, $p$\,$e^+$ \newline
\textbf{Energies:} (820.0, 26.7) GeV \newline
\textbf{Experiment:} H1 (HERA)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2919893}{2919893}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:peter.richardson@durham.ac.uk}{peter.richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys.C63:377-390,1994
  \item DOI: \href{http://dx.doi.org/10.1007/BF01580319}{10.1007/BF01580319}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^- p$ / $e^+ p$ deep inelastic scattering, 820~GeV protons colliding with 26.7~GeV electrons\end{itemize}

\noindent Global properties of the hadronic final state in deep inelastic scattering events at HERA are investigated. The data are corrected for detector effects. Energy flows in both the laboratory frame and the hadronic centre of mass system, and energy-energy correlations in the laboratory frame are presented.  Historically, the Ariadne colour dipole model provided the only satisfactory description of this data, hence making it a useful 'target' analysis for MC shower models.

\clearpage


\clearpage

\typeout{Handling analysis H1_2000_S4129130}\subsection[H1\_2000\_S4129130]{H1\_2000\_S4129130\,\cite{Adloff:1999ws}}
\textbf{H1 energy flow in DIS}\newline
\textbf{Beams:} $p$\,$e^+$ \newline
\textbf{Energies:} (820.0, 27.5) GeV \newline
\textbf{Experiment:} H1 (HERA)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4129130}{4129130}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:peter.richardson@durham.ac.uk}{peter.richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Eur.Phys.J.C12:595-607,2000
  \item DOI: \href{http://dx.doi.org/10.1007/s100520000287}{10.1007/s100520000287}
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/9907027v1}{hep-ex/9907027v1}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ p$ deep inelastic scattering with $p$ at 820 GeV, $e^+$ at 27.5 GeV \ensuremath{\to} \ensuremath{\sqrt{s}} = 300 GeV\end{itemize}

\noindent Measurements of transverse energy flow for neutral current deep- inelastic scattering events produced in positron-proton collisions at HERA. The kinematic range covers squared momentum transfers $Q^2$ from 3.2 to 2200 GeV$^2$; the Bjorken scaling variable $x$ from $8 \times 10^{-5}$ to 0.11 and the hadronic mass $W$ from 66 to 233 GeV. The transverse energy flow is measured in the hadronic centre of mass frame and is studied as a function of $Q^2$, $x$, $W$ and pseudorapidity. The behaviour of the mean transverse energy in the central pseudorapidity region and an interval corresponding to the photon fragmentation region are analysed as a function of $Q^2$ and $W$.  This analysis is useful for exploring the effect of photon PDFs and for tuning models of parton evolution and treatment of fragmentation and the proton remnant in DIS.

\clearpage


\section{RHIC analyses}\typeout{Handling analysis STAR_2006_S6500200}\subsection[STAR\_2006\_S6500200]{STAR\_2006\_S6500200\,\cite{Adams:2006nd}}
\textbf{Identified hadron spectra in pp at 200 GeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (100.0, 100.0) GeV \newline
\textbf{Experiment:} STAR (RHIC pp 200 GeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6500200}{6500200}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Bedanga Mohanty $\langle\,$\href{mailto:bedanga@rcf.bnl.gov}{bedanga@rcf.bnl.gov}$\,\rangle$
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Lett. B637, 161
  \item nucl-ex/0601033
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp at 200 GeV\end{itemize}

\noindent \pT distributions of charged pions and (anti)protons in pp collisions at $\sqrt{s} = 200$ GeV, measured by the STAR experiment at RHIC in non-single-diffractive minbias events.

\clearpage


\clearpage

\typeout{Handling analysis STAR_2006_S6860818}\subsection[STAR\_2006\_S6860818]{STAR\_2006\_S6860818\,\cite{Abelev:2006cs}}
\textbf{Strange particle production in pp at 200 GeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (100.0, 100.0) GeV \newline
\textbf{Experiment:} STAR (RHIC pp 200 GeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6860818}{6860818}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rev. C75, 064901
  \item nucl-ex/0607033
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp at 200 GeV\end{itemize}

\noindent \pT distributions of identified strange particles in pp collisions at $\sqrt{s} = 200$ GeV, measured by the STAR experiment at RHIC in non-single-diffractive minbias events. WARNING The $\langle \pT \rangle$ vs. particle mass plot is not validated yet and might be wrong.

\clearpage


\clearpage

\typeout{Handling analysis STAR_2006_S6870392}\subsection[STAR\_2006\_S6870392]{STAR\_2006\_S6870392\,\cite{Abelev:2006uq}}
\textbf{Inclusive jet cross-section in pp at 200 GeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (100.0, 100.0) GeV \newline
\textbf{Experiment:} STAR (RHIC pp 200 GeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6870392}{6870392}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Rev. Lett. 97, 252001
  \item hep-ex/0608030
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp at 200 GeV\end{itemize}

\noindent Inclusive jet cross section as a function of \pT in pp collisions at $\sqrt{s} = 200$ GeV, measured by the STAR experiment at RHIC.

\clearpage


\clearpage

\typeout{Handling analysis STAR_2009_UE_HELEN}\subsection{STAR\_2009\_UE\_HELEN}
\textbf{UE measurement in pp at 200 GeV}\newline
\textbf{Beams:} $p$\,$p$ \newline
\textbf{Energies:} (100.0, 100.0) GeV \newline
\textbf{Experiment:} STAR (RHIC pp 200 GeV)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+None}{None}\newline
\textbf{Status:} PRELIMINARY\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Helen Caines $\langle\,$\href{mailto:helen.caines@yale.edu}{helen.caines@yale.edu}$\,\rangle$
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item arXiv: \href{http://arxiv.org/abs/0910.5203}{0910.5203}
  \item arXiv: \href{http://arxiv.org/abs/0907.3460}{0907.3460}
  \item WARNING! Mark as "STAR preliminary" and contact authors when using it!
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item pp at 200 GeV\end{itemize}

\noindent UE analysis similar to Rick Field's leading jet analysis. SIScone with radius/resolution parameter R=0.7 is used. Particles with $\pT > 0.2~\text{GeV}$ and $|\eta| < 1$ are included in the analysis. All particles are assumed to have zero mass. Only jets with neutral energy $< 0.7$ are included. For the transMIN and transMAX $\Delta(\phi)$ is between $\pi/3$ and $2\pi/3$, and $\Delta(\eta) < 2.0$. For the jet region the area of the jet is used for the normalization, i.e. the scaling factor is $\pi R^2$ and not $\mathrm{d}\phi\mathrm{d}\eta$ (this is different from what Rick Field does!). The tracking efficiency is $\sim 0.8$, but that is an approximation, as below $\pT \sim 0.6~\text{GeV}$ it is falling quite steeply.

\clearpage


\section{Monte Carlo analyses}\typeout{Handling analysis MC_DIPHOTON}\subsection{MC\_DIPHOTON}
\textbf{Monte Carlo validation observables for diphoton production at LHC}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item LHC pp \ensuremath{\to} jet+jet, photon+jet, photon+photon, all with EW+QCD shower\end{itemize}

\noindent Different observables related to the two photons

\clearpage


\clearpage

\typeout{Handling analysis MC_GENERIC}\subsection{MC\_GENERIC}
\textbf{Generic MC testing analysis}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Ian Bruce $\langle\,$\href{mailto:ibruce@cern.ch}{ibruce@cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Any!\end{itemize}

\noindent Generic analysis of typical event distributions such as $\eta$, $y$, $\pT$, $\phi$\dots

\clearpage


\clearpage

\typeout{Handling analysis MC_HINC}\subsection{MC\_HINC}
\textbf{Monte Carlo validation observables for $h[\tau^+ \, \tau^-]$ production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $h [\to \tau^+ \tau^-]$.\end{itemize}

\noindent Monte Carlo validation observables for $h[\tau^+ \, \tau^-]$ production

\clearpage


\clearpage

\typeout{Handling analysis MC_HJETS}\subsection{MC\_HJETS}
\textbf{Monte Carlo validation observables for $h[\tau^+ \, \tau^-]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $h [\to \tau^+ \tau^-]$ + jets.\end{itemize}

\noindent The available observables are the Higgs mass, \pT of jets 1--4, jet multiplicity, $\Delta\eta(h, \text{jet1})$, $\Delta R(\text{jet2}, \text{jet3})$, differential jet rates 0\ensuremath{\to}1, 1\ensuremath{\to}2, 2\ensuremath{\to}3, 3\ensuremath{\to}4, and integrated 0--4 jet rates.

\clearpage


\clearpage

\typeout{Handling analysis MC_HKTSPLITTINGS}\subsection{MC\_HKTSPLITTINGS}
\textbf{Monte Carlo validation observables for $h[\tau^+ \, \tau^-]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $h [\to \tau^+ \tau^-]$ + jets.\end{itemize}

\noindent Monte Carlo validation observables for $h[\tau^+ \, \tau^-]$ + jets production

\clearpage


\clearpage

\typeout{Handling analysis MC_IDENTIFIED}\subsection{MC\_IDENTIFIED}
\textbf{MC testing analysis for identified particle distributions}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Any!\end{itemize}

\noindent Plotting of distributions of PID codes (all/stable/unstable) and ID-specific distributions such as the $|\eta|$ of $K$, $\pi$ and $\Lambda$ mesons.

\clearpage


\clearpage

\typeout{Handling analysis MC_JETS}\subsection{MC\_JETS}
\textbf{Monte Carlo validation observables for jet production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Pure QCD jet production events at an arbitrary collider.\end{itemize}

\noindent Jets with $p_\perp>20$ GeV are constructed with a $k_\perp$ jet finder with $D=0.7$ and projected onto many different observables.

\clearpage


\clearpage

\typeout{Handling analysis MC_LEADJETUE}\subsection{MC\_LEADJETUE}
\textbf{Underlying event in leading jet events, extended to LHC}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item LHC pp QCD interactions at 0.9, 10 or 14 TeV. Particles with $c \tau > 10$ mm should be set stable. Several $p_\perp^\text{min}$ cutoffs are probably required to fill the profile histograms.\end{itemize}

\noindent Rick Field's measurement of the underlying event in leading jet events, extended to the LHC. As usual, the leading jet of the defines an azimuthal toward/transverse/away decomposition, in this case the event is accepted within $|\eta| < 2$, as in the CDF 2008 version of the analysis. Since this isn't the Tevatron, I've chosen to use $k_\perp$ rather than midpoint jets.

\clearpage


\clearpage

\typeout{Handling analysis MC_PDFS}\subsection{MC\_PDFS}
\textbf{Analysis to study PDF sampling in any MC run}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Any!\end{itemize}

\noindent Plotting of PDF sampling info, such as the $Q^2$ and both $x$ values of the sampling (aggregated and distinguished as max/min, and some correlations with event properties.

\clearpage


\clearpage

\typeout{Handling analysis MC_PHOTONINC}\subsection{MC\_PHOTONINC}
\textbf{Monte Carlo validation observables for single isolated photon production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Tevatron Run II ppbar \ensuremath{\to} gamma + jets.\end{itemize}

\noindent Monte Carlo validation observables for single isolated photon production

\clearpage


\clearpage

\typeout{Handling analysis MC_PHOTONJETS}\subsection{MC\_PHOTONJETS}
\textbf{Monte Carlo validation observables for photon + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Tevatron Run II ppbar \ensuremath{\to} gamma + jets.\end{itemize}

\noindent Different observables related to the photon and extra jets.

\clearpage


\clearpage

\typeout{Handling analysis MC_PHOTONKTSPLITTINGS}\subsection{MC\_PHOTONKTSPLITTINGS}
\textbf{Monte Carlo validation observables for photon + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Tevatron Run II ppbar \ensuremath{\to} gamma + jets.\end{itemize}

\noindent Monte Carlo validation observables for photon + jets production

\clearpage


\clearpage

\typeout{Handling analysis MC_PHOTONS}\subsection{MC\_PHOTONS}
\textbf{Monte Carlo validation observables for general photons}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Steve Lloyd
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Any event type, but there are many observables for photons associated to (semi-)hard leptons.\end{itemize}

\noindent Observables for testing general unisolated photon properties, especially those associated with charged leptons (e and mu).

\clearpage


\clearpage

\typeout{Handling analysis MC_PRINTEVENT}\subsection{MC\_PRINTEVENT}
\textbf{Print out a dump of each event to standard output}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Can be used with any event type.\end{itemize}

\noindent Print out a dump of the event structure to the terminal standard output, in a conveniently human readable form with e.g. particle names in addition to the usual numerical ID codes.

\clearpage


\clearpage

\typeout{Handling analysis MC_QCD_PARTONS}\subsection{MC\_QCD\_PARTONS}
\textbf{Generic parton-level Monte Carlo validation analysis for <X> + jets.}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Any <X> + jets.\end{itemize}

\noindent Only partons (excluding top quarks) are taken into account to construct a kt cluster sequence. Thus this analysis can be used as a generic validation tool for QCD activity.

\clearpage


\clearpage

\typeout{Handling analysis MC_SUSY}\subsection{MC\_SUSY}
\textbf{Validate generic SUSY events, including various lepton invariant mass}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item SUSY events at any energy. \pT cutoff at 10 GeV may be advised.\end{itemize}

\noindent Analysis of generic SUSY events at the LHC, based on Atlas Herwig++ validation analysis contents. Plotted are eta, phi and \pT observables for charged tracks, photons, isolated photons, electrons, muons, and jets, as well as various dilepton mass `edge' plots for different event selection criteria.

\clearpage


\clearpage

\typeout{Handling analysis MC_TTBAR}\subsection{MC\_TTBAR}
\textbf{MC analysis for ttbar studies}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
  \item Dave Mallows
  \item Michal Kawalec
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item * For Pythia6, set MSEL=6 and fix $W^+$ and $W^-$ decays to semi-leptonic modes via the MDME array.
  \item For Fortran Herwig/Jimmy select IPROC=1706.\end{itemize}

\noindent This is a pure Monte Carlo study for semi-leptonic $t\bar{t}$ production.

\clearpage


\clearpage

\typeout{Handling analysis MC_VH2BB}\subsection{MC\_VH2BB}
\textbf{MC unboosted VH2bb validation plots}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} UNVALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Ben Smart $\langle\,$\href{mailto:bsmart@cern.ch}{bsmart@cern.ch}$\,\rangle$
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $VH$ with $H \to b \bar{b}$ and the vector boson decaying to electron or muon channels.\end{itemize}

\noindent Various plots for characterising the process $V H \to b\bar{b}$

\clearpage


\clearpage

\typeout{Handling analysis MC_WINC}\subsection{MC\_WINC}
\textbf{Monte Carlo validation observables for inclusive $W[e \, \nu]$ production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e \, \nu$ + jets analysis.\end{itemize}

\noindent Monte Carlo validation observables for inclusive $W[e \, \nu]$ production

\clearpage


\clearpage

\typeout{Handling analysis MC_WJETS}\subsection{MC\_WJETS}
\textbf{Monte Carlo validation observables for $W[e \, \nu]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e \, \nu$ + jets analysis.\end{itemize}

\noindent Monte Carlo validation observables for $W[e \, \nu]$ + jets production

\clearpage


\clearpage

\typeout{Handling analysis MC_WKTSPLITTINGS}\subsection{MC\_WKTSPLITTINGS}
\textbf{Monte Carlo validation observables for $k_\perp$ splitting scales in $W[e \, \nu]$ + jets events}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e \, \nu$ + jets analysis.\end{itemize}

\noindent Monte Carlo validation observables for $k_\perp$ splitting scales in $W[e \, \nu]$ + jets events

\clearpage


\clearpage

\typeout{Handling analysis MC_WPOL}\subsection{MC\_WPOL}
\textbf{Monte Carlo validation observables for $W$ polarisation}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $W \to e \, \nu$ + jets.\end{itemize}

\noindent Observables sensitive to the polarisation of the W boson: A0, ... A7, fR, fL, f0, separately for W+ and W-.

\clearpage


\clearpage

\typeout{Handling analysis MC_WWINC}\subsection{MC\_WWINC}
\textbf{Monte Carlo validation observables for $W^+[e^+ \, \nu]W^-[\mu^- \, \nu]$ production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $WW$ analysis.\end{itemize}

\noindent Monte Carlo validation observables for $W^+[e^+ \, \nu]W^-[\mu^- \, \nu]$ production

\clearpage


\clearpage

\typeout{Handling analysis MC_WWJETS}\subsection{MC\_WWJETS}
\textbf{Monte Carlo validation observables for $W^+[e^+ \, \nu]W^-[\mu^- \, \nu]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $WW$ + jets analysis.\end{itemize}

\noindent In addition to the typical jet observables this analysis contains observables related to properties of the WW-pair momentum, correlations between the WW, properties of the W bosons, properties of the leptons, correlations between the opposite charge leptons and correlations with jets.

\clearpage


\clearpage

\typeout{Handling analysis MC_WWKTSPLITTINGS}\subsection{MC\_WWKTSPLITTINGS}
\textbf{Monte Carlo validation observables for $W^+[e^+ \, \nu]W^-[\mu^- \, \nu]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $WW$ + jets analysis.\end{itemize}

\noindent Monte Carlo validation observables for $W^+[e^+ \, \nu]W^-[\mu^- \, \nu]$ + jets production

\clearpage


\clearpage

\typeout{Handling analysis MC_XS}\subsection{MC\_XS}
\textbf{MC analysis for process total cross section}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Marek Schoenherr $\langle\,$\href{mailto:marek.schoenherr@tu-dresden.de}{marek.schoenherr@tu-dresden.de}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Suitable for any process.\end{itemize}

\noindent Analysis for bookkeeping of the total cross section, number of generated events and the ratio of events with positive and negative weights.

\clearpage


\clearpage

\typeout{Handling analysis MC_ZINC}\subsection{MC\_ZINC}
\textbf{Monte Carlo validation observables for $Z[e^+ \, e^-]$ production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis. Needs mass cut on lepton pair to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV\end{itemize}

\noindent Monte Carlo validation observables for $Z[e^+ \, e^-]$ production

\clearpage


\clearpage

\typeout{Handling analysis MC_ZJETS}\subsection{MC\_ZJETS}
\textbf{Monte Carlo validation observables for $Z[e^+ \, e^-]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ + jets analysis. Needs mass cut on lepton pair to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV\end{itemize}

\noindent Available observables are Z mass, \pT of jets 1-4, jet multiplicity, $\Delta\eta(Z, \text{jet1})$, $\Delta R(\text{jet2}, \text{jet3})$, differential jet rates 0\ensuremath{\to}1, 1\ensuremath{\to}2, 2\ensuremath{\to}3, 3\ensuremath{\to}4, integrated 0--4 jet rates.

\clearpage


\clearpage

\typeout{Handling analysis MC_ZKTSPLITTINGS}\subsection{MC\_ZKTSPLITTINGS}
\textbf{Monte Carlo validation observables for $Z[e^+ \, e^-]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ + jets analysis. Needs mass cut on lepton pair to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV\end{itemize}

\noindent Monte Carlo validation observables for $Z[e^+ \, e^-]$ + jets production

\clearpage


\clearpage

\typeout{Handling analysis MC_ZZINC}\subsection{MC\_ZZINC}
\textbf{Monte Carlo validation observables for $Z[e^+ \, e^-]Z[\mu^+ \, \mu^-]$ production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $ZZ$ + jets analysis. Needs mass cut on lepton pairs to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV\end{itemize}

\noindent Monte Carlo validation observables for $Z[e^+ \, e^-]Z[\mu^+ \, \mu^-]$ production

\clearpage


\clearpage

\typeout{Handling analysis MC_ZZJETS}\subsection{MC\_ZZJETS}
\textbf{Monte Carlo validation observables for $Z[e^+ \, e^-]Z[\mu^+ \, \mu^-]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $ZZ$ + jets analysis. Needs mass cut on lepton pairs to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV\end{itemize}

\noindent In addition to the typical jet observables this analysis contains observables related to properties of the ZZ-pair momentum, correlations between the ZZ, properties of the Z bosons, properties of the leptons, correlations between the opposite charge leptons and correlations with jets.

\clearpage


\clearpage

\typeout{Handling analysis MC_ZZKTSPLITTINGS}\subsection{MC\_ZZKTSPLITTINGS}
\textbf{Monte Carlo validation observables for $Z[e^+ \, e^-]Z[\mu^+ \, \mu^-]$ + jets production}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Frank Siegert $\langle\,$\href{mailto:frank.siegert@cern.ch}{frank.siegert@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $ZZ$ + jets analysis. Needs mass cut on lepton pairs to avoid photon singularity, e.g. a min range of $66 < m_{ee} < 116$ GeV\end{itemize}

\noindent Monte Carlo validation observables for $Z[e^+ \, e^-]Z[\mu^+ \, \mu^-]$ + jets production

\clearpage


\section{Example analyses}\typeout{Handling analysis EXAMPLE}\subsection{EXAMPLE}
\textbf{A demo to show aspects of writing a Rivet analysis}\newline
\textbf{Beams:} $*$\,$*$ \newline
\textbf{Status:} EXAMPLE\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Andy Buckley $\langle\,$\href{mailto:andy.buckley@cern.ch}{andy.buckley@cern.ch}$\,\rangle$
\end{itemize}
\textbf{No references listed}\\ 
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item All event types will be accepted.\end{itemize}

\noindent This analysis is a demonstration of the Rivet analysis structure and functionality: booking histograms; the initialisation, analysis and finalisation phases; and a simple loop over event particles. It has no physical meaning, but can be used as a simple pedagogical template for writing real analyses.

\clearpage


\section{Misc. analyses}\typeout{Handling analysis ARGUS_1993_S2653028}\subsection[ARGUS\_1993\_S2653028]{ARGUS\_1993\_S2653028\,\cite{Albrecht:1992qf}}
\textbf{Inclusive production of charged pions, kaons and protons in $\Upsilon(4S)$ decays.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (5.3, 5.3) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2653028}{2653028}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys. C58 (1993) 191-198
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis on the $\Upsilon(4S)$ resonance.\end{itemize}

\noindent Measurement of inclusive production of charged pions, kaons and protons from $\Upsilon(4S)$ decays. Kaon spectra are determined in two different ways using particle identification and detecting decays in-flight. Results are background continuum subtracted. This analysis is useful for tuning $B$ meson decay modes.

\clearpage


\clearpage

\typeout{Handling analysis ARGUS_1993_S2669951}\subsection[ARGUS\_1993\_S2669951]{ARGUS\_1993\_S2669951\,\cite{Albrecht:1992nu}}
\textbf{Production of the $\eta'(958)$ and $f_0(980)$ in $e^+e^-$ annihilation in the Upsilon region.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (4.7, 4.7), (5.0, 5.0), (5.2, 5.2) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2669951}{2669951}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys. C58 (1993) 199-206
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis near the $\Upsilon(4S)$ resonance.\end{itemize}

\noindent Measurement of the inclusive production of the $\eta'(958)$ and $f_0(980)$ mesons in $e^+e^-$ annihilation in the Upsilon region. Data are taken on the $\Upsilon(1S)$, $\Upsilon(2S)$ and $\Upsilon(4S)$ resonances and in the nearby continuum (9.36 to 10.45 GeV cm energy)

\clearpage


\clearpage

\typeout{Handling analysis ARGUS_1993_S2789213}\subsection[ARGUS\_1993\_S2789213]{ARGUS\_1993\_S2789213\,\cite{Albrecht:1993fs}}
\textbf{Inclusive production of $K^*(892)$, $\rho^0(770)$, and $\omega(783)$ mesons in the upsilon energy region.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (4.7, 4.7), (5.2, 5.2), (5.3, 5.3) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2789213}{2789213}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys. C61 (1994) 1-18
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis in the 10 GeV CMS energy range\end{itemize}

\noindent Measurement of the inclusive production of the vector mesons $K^*(892)$, $\rho^0(770)$ and $\omega(783)$ in $e^+e^-$ annihilation in the Upsilon region by the Argus Collaboration. Useful for tuning simulations of B meson and bottomium decays.

\clearpage


\clearpage

\typeout{Handling analysis BABAR_2003_I593379}\subsection[BABAR\_2003\_I593379]{BABAR\_2003\_I593379\,\cite{Aubert:2002hc}}
\textbf{Measurement of inclusive charmonium production}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (3.5, 8.0) GeV \newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev. D67 032002, 2003
  \item hep-ex/0207097
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Production of charmionum at the $\Upsilon(4S)$ resonace.\end{itemize}

\noindent Measurement of  $J/\psi$, $\psi'$, $\chi_{c1}$ and $\chi_{c2}$ production using a data sample corresponding to an integrated luminosity of 20.3\;fb$^{-1}$ collected with the BABAR detector at the SLAC PEP-II electron-positron storage ring operating at a centre-of-mass energy near 10.58\;GeV.

\clearpage


\clearpage

\typeout{Handling analysis BABAR_2005_S6181155}\subsection[BABAR\_2005\_S6181155]{BABAR\_2005\_S6181155\,\cite{Aubert:2005cu}}
\textbf{Production and decay of $\Xi^0_c$ at BABAR.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (3.5, 8.0), (3.5, 7.9) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6895344}{6895344}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett. 95 (2005) 142003
  \item hep-ex/0504014
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis on the $\Upsilon(4S)$ resonance, with CoM boost -- 8.0~GeV~($e^−$) and 3.5~GeV~($e^+$)\end{itemize}

\noindent Analysis of $\Xi_c^0$ production in B decays and from the $c\bar{c}$ continuum, with the $\Xi_c^0$ decaying into $\Omega^- K^+$ and $\Xi^- \pi^+$ final states measured using 116.1 $\text{fb}^{-1}$ of data collected by the BABAR detector. The normalisation of the data as been modifed from that presented in the original paper in order to produce a differential cross section rather than the cross section in each bin. In addition to the data presented in the paper plots are alos made with unit normalisation which can be more useful for Monte Carlo tuning.

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\typeout{Handling analysis BABAR_2007_S6895344}\subsection[BABAR\_2007\_S6895344]{BABAR\_2007\_S6895344\,\cite{Aubert:2006cp}}
\textbf{Inclusive $\Lambda_c^+$ Production in $e^+e^-$ Annihilation at $\sqrt{s}=10.54$ GeV and in $\Upsilon(4S)$ Decays.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (3.5, 8.0), (3.5, 7.9) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6895344}{6895344}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev. D75 (2007) 012003
  \item hep-ex/0609004
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis on the $\Upsilon(4S)$ resonance, with CoM boost -- 8.0~GeV~($e^−$) and 3.5~GeV~($e^+$)\end{itemize}

\noindent Measurements of the total production rates and momentum distributions of the charmed baryon $\Lambda_c^+$ in $e^+e^- \to$ hadrons at a centre-of-mass energy of 10.54 GeV and in $\Upsilon(4S)$ decays.

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\typeout{Handling analysis BABAR_2007_S7266081}\subsection[BABAR\_2007\_S7266081]{BABAR\_2007\_S7266081\,\cite{Aubert:2007mh}}
\textbf{Measurements of Semi-Leptonic Tau Decays into Three Charged Hadrons}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (3.5, 8.0) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7266081}{7266081}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.Lett.100:011801,2008
  \item arXiv: \href{http://arxiv.org/abs/0707.2981}{0707.2981}
  \item SLAC-R-936
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Tau production, can be any process but original data was in  $e^+ e^-$ at the $\Upsilon(4S)$ resonance, with CoM boost -- 8.0~GeV~($e^−$) and 3.5~GeV~($e^+$)\end{itemize}

\noindent Measurement of tau decays to three charged hadrons using a data sample corresponding to an integrated luminosity of 342 $fb^{-1}$ collected with the BABAR detector at the SLAC PEP-II electron-positron storage ring operating at a center-of-mass energy near 10.58 GeV.

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\typeout{Handling analysis BELLE_2001_S4598261}\subsection[BELLE\_2001\_S4598261]{BELLE\_2001\_S4598261\,\cite{Abe:2001hj}}
\textbf{Measurement of inclusive production of neutral pions from $\Upsilon(4S)$ decays.}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (3.5, 8.0) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+4598261}{4598261}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev. D64 (2001) 072001
  \item hep-ex/0103041
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis on the $\Upsilon(4S)$ resonance, with CoM boost -- 8.0~GeV~($e^−$) and 3.5~GeV~($e^+$)\end{itemize}

\noindent Measurement of the mean multiplicity and the momentum spectrum of neutral pions from the decays of the Upsilon(4S) resonance using the Belle detector operating at the KEKB $e^+e^-$ storage ring. Useful for tuning $B$ meson decay models.

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\typeout{Handling analysis BELLE_2006_S6265367}\subsection[BELLE\_2006\_S6265367]{BELLE\_2006\_S6265367\,\cite{Seuster:2005tr}}
\textbf{Charm hadrons from fragmentation and B decays on the $\Upsilon(4S)$}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (3.5, 8.0), (3.5, 7.9) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6265367}{6265367}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Jan Eike von Seggern $\langle\,$\href{mailto:jan.eike.von.seggern@physik.hu-berlin.de}{jan.eike.von.seggern@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D73:032002,2006.
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0506068}{hep-ex/0506068}
  \item DOI: \href{http://dx.doi.org/10.1103/PhysRevD.73.032002}{10.1103/PhysRevD.73.032002}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis on the $\Upsilon(4S)$ resonance, with CoM boost -- 8.0~GeV~($e^−$) and 3.5~GeV~($e^+$)\end{itemize}

\noindent Analysis of charm quark fragmentation at 10.6 GeV, based on a data sample of 103 fb collected by the Belle detector at the KEKB accelerator. Fragmentation into charm is studied for the main charmed hadron ground states, namely $D^0$, $D^+$, $D^+_s$ and $\Lambda_c^+$, as well as the excited states $D^{*0}$ and $D^{*+}$. This analysis can be used to constrain charm fragmentation in Monte Carlo generators. As the original data are not corrected for the branching ratios of the decay modes used to observed the charm hadrons we also include distributions with unit normalisation which are more useful for Monte Carlo tuning.

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\typeout{Handling analysis CLEO_2004_S5809304}\subsection[CLEO\_2004\_S5809304]{CLEO\_2004\_S5809304\,\cite{Artuso:2004pj}}
\textbf{Charm hadrons from fragmentation near the $\Upsilon(4S)$}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (5.3, 5.3) GeV \newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+6265367}{6265367}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Peter Richardson $\langle\,$\href{mailto:Peter.Richardson@durham.ac.uk}{Peter.Richardson@durham.ac.uk}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys.Rev.D70:112001,2004.
  \item arXiv: \href{http://arxiv.org/abs/hep-ex/0402040}{hep-ex/0402040}
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^-$ analysis near the $\Upsilon(4S)$ resonance\end{itemize}

\noindent Analysis of charm quark fragmentation at 10.5 GeV, based on a data sample of 103 fb collected by the CLEO experiment. Fragmentation into charm is studied for the charmed hadron ground states, namely $D^0$, $D^+$, as well as the excited states $D^{*0}$ and $D^{*+}$. This analysis can be used to constrain charm fragmentation in Monte Carlo generators.

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\typeout{Handling analysis JADE_1998_S3612880}\subsection[JADE\_1998\_S3612880]{JADE\_1998\_S3612880\,\cite{MovillaFernandez:1997fr}}
\textbf{Event shapes for 22, 35 and 44 GeV}\newline
\textbf{Beams:} $e^-$\,$e^+$ \newline
\textbf{Energies:} (11.0, 11.0), (17.5, 17.5), (22.0, 22.0) GeV \newline
\textbf{Experiment:} JADE (PETRA)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+3612880}{3612880}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz holger.schulz@physik.hu-berlin.de
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item hep-ex/9708034
  \item Eur.Phys.J.C1:461-478,1998
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Z\ensuremath{\to}hadronic final states, bbar contributions have been corrected for as well as ISR\end{itemize}

\noindent Thrust, Jet Mass and Broadenings, Y23 for 35 and 44 GeV and only Y23 at 22 GeV.

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\typeout{Handling analysis PDG_HADRON_MULTIPLICITIES}\subsection[PDG\_HADRON\_MULTIPLICITIES]{PDG\_HADRON\_MULTIPLICITIES\,\cite{Amsler:2008zzb}}
\textbf{Hadron multiplicities in hadronic $e^+e^-$ events}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (5.0, 5.0), (17.5, 17.5), (45.6, 45.6), (88.5, 88.5) GeV \newline
\textbf{Experiment:} PDG (Various)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7857373}{7857373}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Hendrik Hoeth $\langle\,$\href{mailto:hendrik.hoeth@cern.ch}{hendrik.hoeth@cern.ch}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Lett. B, 667, 1 (2008)
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic events in $e^+ e^-$ collisions\end{itemize}

\noindent Hadron multiplicities in hadronic $e^+e^-$ events, taken from Review of Particle Properties 2008, table 40.1, page 355.   Average hadron multiplicities per hadronic $e^+e^-$ annihilation event at $\sqrt{s} \approx {}$ 10, 29--35, 91, and 130--200 GeV. The numbers are averages from various experiments. Correlations of the systematic uncertainties were considered for the calculation of the averages.

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\typeout{Handling analysis PDG_HADRON_MULTIPLICITIES_RATIOS}\subsection[PDG\_HADRON\_MULTIPLICITIES\_RATIOS]{PDG\_HADRON\_MULTIPLICITIES\_RATIOS\,\cite{Amsler:2008zzb}}
\textbf{Ratios (w.r.t. $\pi^+/\pi^-$) of hadron multiplicities in hadronic $e^+e^-$ events}\newline
\textbf{Beams:} $e^+$\,$e^-$ \newline
\textbf{Energies:} (5.0, 5.0), (17.5, 17.5), (45.6, 45.6), (88.5, 88.5) GeV \newline
\textbf{Experiment:} PDG (Various)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+7857373}{7857373}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz $\langle\,$\href{mailto:holger.schulz@physik.hu-berlin.de}{holger.schulz@physik.hu-berlin.de}$\,\rangle$
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Phys. Lett. B, 667, 1 (2008)
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item Hadronic events in $e^+ e^-$ collisions\end{itemize}

\noindent Ratios (w.r.t. $\pi^+/\pi^-$) of hadron multiplicities in hadronic $e^+ e^-$ events, taken from Review of Particle Properties 2008, table 40.1, page 355.  Average hadron multiplicities per hadronic $e^+ e^-$ annihilation event at $\sqrt{s} \approx$ 10, 29--35, 91, and 130--200 GeV, normalised to the pion multiplicity. The numbers are averages from various experiments. Correlations of the systematic uncertainties were considered for the calculation of the averages.

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\typeout{Handling analysis TASSO_1990_S2148048}\subsection[TASSO\_1990\_S2148048]{TASSO\_1990\_S2148048\,\cite{Braunschweig:1990yd}}
\textbf{Event shapes in e+e- annihilation at 14-44 GeV}\newline
\textbf{Beams:} $e^-$\,$e^+$ \newline
\textbf{Energies:} (7.0, 7.0), (11.0, 11.0), (17.5, 17.5), (21.9, 21.9) GeV \newline
\textbf{Experiment:} TASSO (PETRA)\newline
\textbf{Spires ID:} \href{http://inspire-hep.net/search?p=find+key+2148048}{2148048}\newline
\textbf{Status:} VALIDATED\newline
\textbf{Authors:}
 \penalty 100
\begin{itemize}
  \item Holger Schulz holger.schulz@physik.hu-berlin.de
\end{itemize}
\textbf{References:}
 \penalty 100
\begin{itemize}
  \item Z.Phys.C47:187-198,1990
  \item DESY-90-013
\end{itemize}
\textbf{Run details:}
 \penalty 100
\begin{itemize}

  \item $e^+ e^- \to \text{jet jet}$ (+ jets). Kinematic cuts such as CKIN(1) in Pythia need to be set slightly below the CMS energy.\end{itemize}

\noindent Event shapes Thrust, Sphericity, Aplanarity at four different energies

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