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<H2><A NAME="SECTION00041000000000000000">
3.1 Input data</A>
</H2>

<P>
Input data 
is organized as several namelists, followed by other fields (``cards'')
introduced by keywords. The namelists are

<P>
<TABLE CELLPADDING=3>
<TR><TD ALIGN="LEFT">&amp;CONTROL:</TD>
<TD ALIGN="LEFT">general variables controlling the run</TD>
</TR>
<TR><TD ALIGN="LEFT">&amp;SYSTEM:</TD>
<TD ALIGN="LEFT">structural information on the system under investigation</TD>
</TR>
<TR><TD ALIGN="LEFT">&amp;ELECTRONS:</TD>
<TD ALIGN="LEFT">electronic variables: self-consistency, smearing</TD>
</TR>
<TR><TD ALIGN="LEFT">&amp;IONS (optional):</TD>
<TD ALIGN="LEFT">ionic variables: relaxation, dynamics</TD>
</TR>
<TR><TD ALIGN="LEFT">&amp;CELL (optional):</TD>
<TD ALIGN="LEFT">variable-cell optimization or dynamics</TD>
</TR>
</TABLE>    
<BR>
Optional namelist may be omitted if the calculation to be performed
does not require them. This depends on the value of variable 
<TT>calculation</TT>
in namelist &amp;CONTROL. Most variables in namelists have default values. Only
the following variables in &amp;SYSTEM must always be specified:

<P>
<TABLE CELLPADDING=3>
<TR><TD ALIGN="LEFT"><TT>ibrav</TT></TD>
<TD ALIGN="LEFT">(integer)</TD>
<TD ALIGN="LEFT">Bravais-lattice index</TD>
</TR>
<TR><TD ALIGN="LEFT"><TT>celldm</TT></TD>
<TD ALIGN="LEFT">(real, dimension 6)</TD>
<TD ALIGN="LEFT">crystallographic constants</TD>
</TR>
<TR><TD ALIGN="LEFT"><TT>nat</TT></TD>
<TD ALIGN="LEFT">(integer)</TD>
<TD ALIGN="LEFT">number of atoms in the unit cell</TD>
</TR>
<TR><TD ALIGN="LEFT"><TT>ntyp</TT></TD>
<TD ALIGN="LEFT">(integer)</TD>
<TD ALIGN="LEFT">number of types of atoms in the unit cell</TD>
</TR>
<TR><TD ALIGN="LEFT"><TT>ecutwfc</TT></TD>
<TD ALIGN="LEFT">(real)</TD>
<TD ALIGN="LEFT">kinetic energy cutoff (Ry) for wavefunctions.</TD>
</TR>
</TABLE>    
<BR>
For metallic systems, you have to specify how metallicity is treated
in
variable <TT>occupations</TT>. If you choose <TT>occupations='smearing'</TT>,
you have
to specify the smearing type <TT>smearing</TT> and the smearing width 
<TT>degauss</TT>. Spin-polarized systems are as a rule treated as metallic 
system, unless the total magnetization, <TT>tot_magnetization</TT>
is set to a fixed value, or if occupation numbers are fixed
(<TT>occupations='from input'</TT> and card OCCUPATIONS).

<P>
Explanations for the meaning of variables <TT>ibrav</TT> and <TT>celldm</TT>,
as well as on alternative ways to input structural data,
are in files <TT>PW/Doc/INPUT_PW.txt</TT> and <TT>PW/Doc/INPUT_PW.html</TT>. 
These files are the reference for input data and describe a large number
of other variables as well. Almost all variables have default 
values, which may or may not fit your needs.

<P>
Comment lines in namelists can be introduced by a "!", exactly as in fortran 
code.

<P>
After the namelists, you have several fields (``cards'')
introduced by keywords with self-explanatory names:
<BLOCKQUOTE>
ATOMIC_SPECIES
<BR>
ATOMIC_POSITIONS
<BR>
K_POINTS
<BR>
CELL_PARAMETERS (optional)
<BR>
OCCUPATIONS (optional)
<BR>
</BLOCKQUOTE>
The keywords may be followed on the same line by an option. Unknown
fields are ignored. 
See the files mentioned above for details on the available ``cards''.

<P>
Comments lines in ``cards'' can be introduced by either a ``!'' or a ``#''
character in the first position of a line.

<P>
Note about k points: The k-point grid can be either automatically generated 
or manually provided as a list of k-points and a weight in the Irreducible
Brillouin Zone only of the Bravais lattice of the crystal. The code will 
generate (unless instructed not to do so: see variable <TT>nosym</TT>) all
required k-points
and weights if the symmetry of the system is lower than the symmetry of the
Bravais lattice. The automatic generation of k-points follows the convention
of Monkhorst and Pack.

<P>
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<ADDRESS>
paolo giannozzi
2014-05-28
</ADDRESS>
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