quantum-espresso/PHonon/Doc/INPUT_Q2R.def

153 lines
5.3 KiB
Modula-2

input_description -distribution {Quantum ESPRESSO} -package PHonon -program q2r.x {
toc {}
intro {
@b {Purpose of q2r.x:}
It reads force constant matrices C(q) produced by the @b ph.x code
for a grid of q-points and calculates the corresponding set
of interatomic force constants (IFC), C(R)
@b {Input data format:} [ ] = it depends
@b {Structure of the input data:}
========================================================================
@b &INPUT
...specs of namelist variables...
@b /
[ nr1 nr2 nr3
nfile
file(1)
file(2)
...
file(nfile) ]
}
namelist INPUT {
var fildyn -type CHARACTER {
status { REQUIRED }
info {
Input file name (must be specified).
@b "fildyn"0 contains information on the q-point grid
@b "fildyn"1-N contain force constants C_n = C(q_n),
where @b {n = 1,...N}, where N is the number of
q-points in the irreducible brillouin zone.
Normally this should be the same as specified on input
to the phonon code.
In the non collinear/spin-orbit case the files
produced by @b ph.x are in .xml format. In this case
@ref fildyn is the same as in the phonon code + the
.xml extension.
}
}
var flfrc -type CHARACTER {
status { REQUIRED }
info {
Output file containing the IFC in real space (must be specified)
}
}
var zasr -type CHARACTER {
default { 'no' }
options {
info {
Indicates the type of Acoustic Sum Rules used for the Born
effective charges.
Allowed values:
}
opt -val 'no' {
no Acoustic Sum Rules imposed (default)
}
opt -val 'simple' {
previous implementation of the asr used
(3 translational asr imposed by correction of
the diagonal elements of the force-constants matrix)
}
opt -val 'crystal' {
3 translational asr imposed by optimized
correction of the IFC (projection)
}
opt -val 'one-dim' {
3 translational asr + 1 rotational asr
imposed by optimized correction of the IFC (the
rotation axis is the direction of periodicity; it
will work only if this axis considered is one of
the cartesian axis).
}
opt -val 'zero-dim' {
3 translational asr + 3 rotational asr
imposed by optimized correction of the IFC.
}
info {
Note that in certain cases, not all the rotational asr
can be applied (e.g. if there are only 2 atoms in a
molecule or if all the atoms are aligned, etc.).
In these cases the supplementary asr are cancelled
during the orthonormalization procedure (see below).
}
}
}
var loto_2d -type LOGICAL {
info {
set to @b .true. to activate two-dimensional treatment
of LO-TO splitting.
}
}
}
choose {
when -test {file {fildyn}0 does not exist} {
message {
If a file @b "fildyn"0 is not found, the code will ignore variable
@ref fildyn and will try to read from the following cards the missing
information on the q-point grid and file names:
}
linecard {
vargroup -type INTEGER {
var nr1
var nr2
var nr3
info {
dimensions of the FFT grid formed by the q-point grid
}
}
}
card fileSpecs -nameless 1 {
syntax {
line {
var nfile -type INTEGER {
info {
number of files containing C(q_n), n=1,@ref nfile
}
}
}
table file_n {
rows -start 1 -end nfile {
col file -type CHARACTER {
info {
names of the files containing C(q_n), n=1,@ref nfile
Note that the name and order of files is not important as
long as @b {q=0 is the first}.
}
}
}
}
}
}
}
}
}