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<?xml version="1.0" encoding="ISO-8859-1"?>
<?xml-stylesheet type="text/xsl" href="input_xx.xsl"?>
<!-- FILE AUTOMATICALLY CREATED: DO NOT EDIT, CHANGES WILL BE LOST -->
<input_description distribution="Quantum Espresso" package="PWscf" program="pwcond.x" >
<toc>
</toc>
<intro>
This program computes the transmittance of a system and/or its
complex band structure.
It is controlled through the following variables
in the namelist inputcond.
Structure of the input data:
============================
&INPUTCOND
...
/
</intro>
<namelist name="INPUTCOND" >
<var name="outdir" type="CHARACTER" >
<info>
temporary directory (as in PWscf)
</info>
</var>
<var name="prefixt" type="CHARACTER" >
<info>
prefix for the file (as in PWscf) containing all the
regions (left lead + scatt. reg. + right lead)
</info>
</var>
<var name="prefixl" type="CHARACTER" >
<info>
prefix for the file containing only the left lead
</info>
</var>
<var name="prefixs" type="CHARACTER" >
<info>
prefix for the file containing the scattering region
</info>
</var>
<var name="prefixr" type="CHARACTER" >
<info>
prefix for the file containing only the right lead
</info>
</var>
<var name="tran_prefix" type="CHARACTER" >
<default> none
</default>
<see> recover
</see>
<info>
if tran_prefix is specified the program will save partial results
of a transmission calculation (ikind .GE. 1) in a specific
directory (outdir/tran_prefix.cond_save)
</info>
</var>
<var name="max_seconds" type="REAL" >
<default> 1.D+7, or 150 days, i.e. no time limit
</default>
<see> tran_prefix
</see>
<info>
jobs stops after max_seconds elapsed time (wallclock time).
It can be enabled only if tran_prefix is specified.
</info>
</var>
<var name="recover" type="LOGICAL" >
<default> .FALSE.
</default>
<see> tran_prefix
</see>
<info>
restarts a previously interrupted transmission calculation (only if
tran_prefix was specified). It can also be used to gather partial
results from a calculation that was split by using start_e,last_e
and/or start_k,last_k (see corresponding keywords).
</info>
</var>
<var name="band_file" type="CHARACTER" >
<info>
file on which the complex bands are saved
</info>
</var>
<var name="tran_file" type="CHARACTER" >
<info>
file where the transmission is written
</info>
</var>
<var name="save_file" type="CHARACTER" >
<info>
file where the data necessary for PWCOND are written
so that no prefix files of PW are longer needed
</info>
</var>
<var name="fil_loc" type="CHARACTER" >
<info>
file on/from which the 2D eigenvalue problem data are
saved/read
</info>
</var>
<var name="lwrite_cond" type="LOGICAL" >
<info>
if .t. save the data necessary for PWCOND in save_file
</info>
</var>
<var name="loop_ek" type="LOGICAL" >
<info>
if .t. the energy loop is outside the k-point loop
</info>
</var>
<var name="lread_cond" type="LOGICAL" >
<info>
if .t. read the data necessary for PWCOND from save_file
</info>
</var>
<var name="lwrite_loc" type="LOGICAL" >
<info>
if .t. save 2D eigenvalue problem result in fil_loc
</info>
</var>
<var name="lread_loc" type="LOGICAL" >
<info>
if .t. read 2D eigenvalue problem result from fil_loc
</info>
</var>
<var name="ikind" type="INTEGER" >
<info>
The kind of conductance calculation:
ikind=0 - just complex band structure (CBS) calculation
ikind=1 - conductance calculation with identical
left and right leads
ikind=2 - conductance calculation with different
left and right leads
</info>
</var>
<var name="iofspin" type="INTEGER" >
<info>
spin index for which the calculations are performed
</info>
</var>
<var name="tk_plot" type="INTEGER" >
<info>
if > 0, plot T(kx,ky) at each energy in the region [tk_plot x full BZ]
</info>
</var>
<var name="llocal" type="LOGICAL" >
<info>
if .t. calculations are done with only local part of PP
</info>
</var>
<var name="bdl" type="REAL" >
<info>
right boundary of the left lead (left one is supposed to be at 0)
(in units of lattice parameter "alat" defined in the scf run)
</info>
</var>
<var name="bds" type="REAL" >
<info>
right boundary of the scatt. reg. (left one is at 0 if prefixs
is used and = bdl if prefixt is used)
(in units of lattice parameter "alat" defined in the scf run)
</info>
</var>
<var name="bdr" type="REAL" >
<info>
right boundary of the right lead (left one is at 0 if prefixr
is used and = bds if prefixt is used)
(in units of lattice parameter "alat" defined in the scf run)
</info>
</var>
<var name="nz1" type="INTEGER" >
<info>
the number of subslabs in the slab (to calculate integrals)
</info>
</var>
<var name="energy0" type="REAL" >
<info>
initial energy
</info>
</var>
<var name="denergy" type="REAL" >
<info>
energy step (if denergy=0.0 the energy is read from the list)
</info>
</var>
<var name="nenergy" type="INTEGER" >
<info>
number of energies
WARNING: the energy in input file is given in eV taken from Ef,
and denergy should be negative
</info>
</var>
<var name="start_e" type="INTEGER" >
<default> 1
</default>
<see> last_e
</see>
<info>
if start_e > 1, the scattering problem is solved only for those
energies with index between start_e and last_e in the energy list.
NOTE: start_e <= last_e and start_e <= nenergy must be satisfied
</info>
</var>
<var name="last_e" type="INTEGER" >
<default> nenergy
</default>
<see> start_e
</see>
<info>
index of the last energy to be computed. If last_e > nenergy,
then last_e will be automatically set to nenergy.
</info>
</var>
<var name="start_k" type="INTEGER" >
<default> 1
</default>
<see> last_k
</see>
<info>
if start_k > 1, the scattering problem is solved only for those
k-points with index between start_k and last_k in the k-point list.
In order to recover the full transmission (i.e. integrated over the
full Brillouin Zone) at the end, perform the partial runs specifying
a value for tran_prefix (the restart directory), then put all the
partial transmission files 'transmission_k#_e#' inside a unique
restart directory and run pwcond.x with recover=.TRUE. (without
specifying any value for start_k and last_k).
NOTE: start_k <= last_k must be satisfied and start_k must also
not be greater than the actual number of k-point in the list
(if you compute the grid automatically by specifying the grid
size and shifts, you can use kpoints.x to check that number).
</info>
</var>
<var name="last_k" type="INTEGER" >
<default> nenergy
</default>
<see> start_k
</see>
<info>
index of the last k-point to be computed. If last_k is bigger than the
actual number of points in the list, then it will be set to that number.
</info>
</var>
<var name="ecut2d" type="REAL" >
<info>
2-D cutoff
</info>
</var>
<var name="ewind" type="REAL" >
<info>
the energy window for reduction of 2D plane wave basis set (in XY)
</info>
</var>
<var name="epsproj" type="REAL" >
<info>
accuracy of 2D basis set reduction
</info>
</var>
<var name="orbj_in" type="REAL" >
<info>
the initial orbital for projecting the transmission
</info>
</var>
<var name="orbj_fin" type="REAL" >
<info>
the final orbital for projecting the transmission
</info>
</var>
</namelist>
<card name="K_and_Energy_Points" nameless="1" >
<syntax>
<line>
<var name="nkpts" type="INTEGER" >
<info>
Number of k_\perp points
</info>
</var>
</line>
<table name="k_points" >
<rows start="1" end="nkpts" >
<colgroup type="REAL" >
<col name="kx" >
</col>
<col name="ky" >
</col>
<col name="weight" >
</col>
<info>
k-point coordinates and weights
</info>
</colgroup>
</rows>
</table>
<line>
<var name="nenergy" type="INTEGER" >
<info>
number of energy points
</info>
</var>
</line>
</syntax>
</card>
</input_description>
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