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<H2><A ID="SECTION00023000000000000000">
1.3 Pseudopotential generation, in general</A>
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<EM>In the following I am assuming that the basic PP theory
is known to the reader. Otherwise, see
Refs.[<A
HREF="node21.html#NC">1</A>,<A
HREF="node21.html#BHS">4</A>,<A
HREF="node21.html#TM">7</A>,<A
HREF="node21.html#fhi98PP">8</A>,<A
HREF="node21.html#RRKJ">9</A>] and references quoted
therein for NC-PP's; Refs.[<A
HREF="node21.html#van">2</A>,<A
HREF="node21.html#PAW">3</A>] for US-PP's and PAWsets.
I am also assuming that the generated PP's are to be used
in separable form [<A
HREF="node21.html#KB">10</A>] with a plane-wave (PW) basis set.
</EM>
<P>
<EM>The PP generation is a three-step process. First, one generates
atomic levels and orbitals with Density-functional theory (DFT).
Second, from atomic results one generates the PP. Third, one checks
whether the reesulting PP is actually working. If not, one tries again in
a different way.
</EM>
<P>
<EM>The first step is invariably done assuming a spherically symmetric
self-consistent Hamiltonian, so that all elementary quantum mechanics
results for the atom apply. The atomic state is defined by the
"electronic configuration", one-electron states are defined by a
principal quantum number and by the angular momentum and are obtained
by solving a self-consistent radial Schrödinger-like (Kohn-Sham)
equation.
</EM>
<P>
<EM>The second step exists in many variants. One can generate ``traditional''
single-projector NC-PP's; multiple-projector US-PP's, or PAW sets.
The crucial step is in all cases the generation of smooth
``pseudo-orbitals'' from atomic all-electron (AE) orbitals.
Two popular pseudization
methods are presently implemented: Troullier-Martins [<A
HREF="node21.html#TM">7</A>]
and Rappe-Rabe-Kaxiras-Joannopoulos [<A
HREF="node21.html#RRKJ">9</A>] (RRKJ).
</EM>
<P>
<EM>The second and third steps are closer to cooking than to science.
There is a
large arbitrariness in the preceding step that one would like to
exploit in order to get the "best" PP, but there is no well-defined
way to do this. Moreover one is often forced to strike a compromise
between transferability (thus accuracy) and hardness (i.e. computer
time). These two steps are the main focus of these notes.
</EM>
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