TABLE OF CONTENTS
INTRODUCTION
BEGIN
BEGIN_PATH_INPUT
&PATH
string_method | restart_mode | nstep_path | num_of_images | opt_scheme | CI_scheme | first_last_opt | minimum_image | temp_req | ds | k_max | k_min | path_thr | use_masses | use_freezing | lfcp | fcp_mu | fcp_thr | fcp_scheme
CLIMBING_IMAGES
index1, index2, ... indexN
BEGIN_ENGINE_INPUT
BEGIN_POSITIONS
FIRST_IMAGE
ATOMIC_POSITIONS
TOTAL_CHARGE
tot_charge
INTERMEDIATE_IMAGE
ATOMIC_POSITIONS
TOTAL_CHARGE
tot_charge
LAST_IMAGE
ATOMIC_POSITIONS
TOTAL_CHARGE
tot_charge
INTRODUCTION
Input data format: { } = optional, [ ] = it depends, | = or
All quantities whose dimensions are not explicitly specified are in
RYDBERG ATOMIC UNITS
BEWARE: TABS, DOS <CR><LF> CHARACTERS ARE POTENTIAL SOURCES OF TROUBLE
neb.x DOES NOT READ FROM STANDARD INPUT !
There are two ways for running a calculation with neb.x:
(1) specifying a file to parse with the ./neb.x -inp or ./neb.x -input
command line option.
(2) or specifying the number of copies of PWscf inputs with the ./neb.x -input_images
For case (1) a file containing special KEYWORDS (aka SUPERCARDS) has to be
written (see below). These KEYWORDS tell the parser which part of the file
contains the neb specifics and which part contains the energy/force engine
input (at the moment only PW). After the parsing, different files are
generated: neb.dat, with the neb specific variables, and a set of pw_*.in
PWscf input files, i.e., one for each input position. All options for a
single SCF calculation apply.
The general structure of the file to be parsed is:
==================================================
BEGIN
BEGIN_PATH_INPUT
... neb specific namelists and cards
END_PATH_INPUT
BEGIN_ENGINE_INPUT
...pw specific namelists and cards
BEGIN_POSITIONS
FIRST_IMAGE
...pw ATOMIC_POSITIONS card
...pw TOTAL_CHARGE card (only for FCP)
INTERMEDIATE_IMAGE
...pw ATOMIC_POSITIONS card
...pw TOTAL_CHARGE card (only for FCP)
LAST_IMAGE
...pw ATOMIC_POSITIONS card
...pw TOTAL_CHARGE card (only for FCP)
END_POSITIONS
... other pw specific cards
END_ENGINE_INPUT
END
For case (2) neb.dat and all pw_1.in, pw_2.in ... should be already present.
Structure of the NEB-only input data (file neb.dat):
====================================================
&PATH
...
/
[ CLIMBING_IMAGES
list of images, separated by a comma ]
BEGIN |
Syntax of this supercard is the following:
BEGIN ... content of the supercard here ... END
and the content is:
|
BEGIN_PATH_INPUT |
Syntax of this supercard is the following:
BEGIN_PATH_INPUT ... content of the supercard here ... END_PATH_INPUT
and the content is:
|
Namelist: &PATH
|
string_method |
CHARACTER |
Default: |
'neb'
|
A string describing the task to be performed. Options are:
- 'neb' :
nudget-elastic-band
- 'smd' :
string-method-dynamics
|
restart_mode |
CHARACTER |
Default: |
'from_scratch'
|
Options are:
- 'from_scratch' :
from scratch
- 'restart' :
from previous interrupted run
|
nstep_path |
INTEGER |
Default: |
1
|
number of ionic + electronic steps
|
num_of_images |
INTEGER |
Default: |
0
|
Number of points used to discretize the path
(it must be larger than 3).
|
opt_scheme |
CHARACTER |
Default: |
'quick-min'
|
Specify the type of optimization scheme:
- 'sd' :
steepest descent
- 'broyden' :
quasi-Newton Broyden's second method (suggested)
- 'broyden2' :
another variant of the quasi-Newton Broyden's
second method to be tested and compared with the
previous one.
- 'quick-min' :
an optimisation algorithm based on the
projected velocity Verlet scheme
- 'langevin' :
finite temperature langevin dynamics of the
string (smd only). It is used to compute the
average path and the free-energy profile.
|
CI_scheme |
CHARACTER |
Default: |
'no-CI'
|
Specify the type of Climbing Image scheme:
- 'no-CI' :
climbing image is not used
- 'auto' :
original CI scheme. The image highest in energy
does not feel the effect of springs and is
allowed to climb along the path
- 'manual' :
images that have to climb are manually selected.
See also CLIMBING_IMAGES card
|
first_last_opt |
LOGICAL |
Default: |
.FALSE.
|
Also the first and the last configurations are optimized
"on the fly" (these images do not feel the effect of the springs).
|
minimum_image |
LOGICAL |
Default: |
.FALSE.
|
Assume a "minimum image criterion" to build the path. If an atom
moves by more than half the length of a crystal axis between one
image and the next in the input (before interpolation),
an appropriate periodic replica of that atom is chosen.
Useful to avoid jumps in the initial reaction path.
|
temp_req |
REAL |
Default: |
0.D0 Kelvin
|
Temperature used for the langevin dynamics of the string.
|
ds |
REAL |
Default: |
1.D0
|
Optimisation step length ( Hartree atomic units ).
If opt_scheme=="broyden", ds is used as a guess for the
diagonal part of the Jacobian matrix.
|
k_max, k_min |
REAL |
Default: |
0.1D0 Hartree atomic units
|
Set them to use a Variable Elastic Constants scheme
elastic constants are in the range [ k_min, k_max ]
this is useful to rise the resolution around the saddle point.
|
path_thr |
REAL |
Default: |
0.05D0 eV / Angstrom
|
The simulation stops when the error ( the norm of the force
orthogonal to the path in eV/A ) is less than path_thr.
|
use_masses |
LOGICAL |
Default: |
.FALSE.
|
If. TRUE. the optimisation of the path is performed using
mass-weighted coordinates. Useful together with quick-min
optimization scheme, if some bonds are much stiffer than
others. By assigning a larger (fictitious) mass to atoms
with stiff bonds, one may use a longer time step "ds"
|
use_freezing |
LOGICAL |
Default: |
.FALSE.
|
If. TRUE. the images are optimised according to their error:
only those images with an error larger than half of the largest
are optimised. The other images are kept frozen.
|
lfcp |
LOGICAL |
Default: |
.FALSE.
|
See: |
fcp_mu |
If .TRUE. perform a constant bias potential (constant-mu)
calculation with ESM method (assume_isolated = 'esm' and
esm_bc = 'bc2' or 'bc3' must be set in SYSTEM namelist).
fcp_mu gives the target Fermi energy.
See the header of PW/src/fcp_module.f90 for documentation
|
fcp_mu |
REAL |
Default: |
0.d0
|
See: |
lfcp |
If lfcp == .TRUE., gives the target Fermi energy [eV].
One can specify the total charge of the system for the first
and last image by giving TOTAL_CHARGE cards
so that the Fermi energy of these systems will be the target value,
otherwise first_last_opt should be .TRUE.
For the initial charge of intermediate images, the TOTAL_CHARGE
is linearly interpolated between the initial and the final ones
unless the TOTAL_CHARGE is given in the input file.
|
fcp_thr |
REAL |
Default: |
0.01D0 V
|
See: |
lfcp |
The simulation stops when the error ( the maximum of the force
acting on the FCP in V ) is less than fcp_thr.
|
fcp_scheme |
CHARACTER |
Default: |
'lm'
|
See: |
lfcp |
Specify the type of optimization scheme for FCP:
- 'lm' :
Line-Minimization method.
- 'newton' :
Newton-Raphson method with diagonal hessian matrix.
Also, coupling with DIIS.
- 'coupled' :
Coupled method with ionic positions.
This is available only if opt_scheme == 'broyden',
or 'broyden2'.
|
|
|
Card: CLIMBING_IMAGES |
Optional card, needed only if CI_scheme == 'manual', ignored otherwise !
Syntax:
CLIMBING_IMAGES
|
Description of items:
index1, index2, ... indexN
|
INTEGER |
index1, index2, ..., indexN are indices of the images to which the
Climbing-Image procedure apply. If more than one image is specified
they must be separated by a comma.
|
|
|
|
END_PATH_INPUT |
BEGIN_ENGINE_INPUT |
Syntax of this supercard is the following:
BEGIN_ENGINE_INPUT ... content of the supercard here ... END_ENGINE_INPUT
and the content is:
|
Here comes the pw.x specific namelists and cards (see file: INPUT_PW.html or INPUT_PW.txt)
with the exception of ATOMIC_POSITIONS cards, which are specified separately within the
BEGIN_POSITIONS/END_POSITIONS supercard as described below.
So the input that follows here is of the following structure:
&CONTROL
...
/
&SYSTEM
...
/
&ELECTRONS
...
/
...
BEGIN_POSITIONS |
Syntax of this supercard is the following:
BEGIN_POSITIONS ... content of the supercard here ... END_POSITIONS
and the content is:
|
NB:
Atomic positions for all the images are specified within the BEGIN_POSITIONS / END_POSITIONS
supercard, where each instance of ATOMIC_POSITIONS card is prefixed either by FIRST_IMAGE,
INTERMEDIATE_IMAGE, or LAST_IMAGE keywords.
IF lfcp == .TRUE., total charges for all images have to be specified with TOTAL_CHARGE cards.
Note that intermediate images are optional, i.e., there can be none or any number of
INTERMEDIATE_IMAGE images.
FIRST_IMAGE |
Syntax of this supercard is the following:
FIRST_IMAGE ... content of the supercard here ...
and the content is:
|
Card: ATOMIC_POSITIONS { alat | bohr | angstrom | crystal | crystal_sg } |
For the description of ATOMIC_POSITIONS card see file: INPUT_PW.html or INPUT_PW.txt
|
|
Card: TOTAL_CHARGE |
Optional card, needed only if lfcp == .TRUE.
Syntax:
TOTAL_CHARGE
|
Description of items:
tot_charge
|
REAL |
tot_charge is the total charge of the system.
|
|
|
|
INTERMEDIATE_IMAGE |
Syntax of this supercard is the following:
INTERMEDIATE_IMAGE ... content of the supercard here ...
and the content is:
|
( Remark: There can be any number (including zero) of INTERMEDIATE_IMAGE supercards. ) |
Card: ATOMIC_POSITIONS { alat | bohr | angstrom | crystal | crystal_sg } |
For the description of ATOMIC_POSITIONS card see file: INPUT_PW.html or INPUT_PW.txt
|
|
Card: TOTAL_CHARGE |
Optional card, needed only if lfcp == .TRUE.
Syntax:
TOTAL_CHARGE
|
Description of items:
tot_charge
|
REAL |
tot_charge is the total charge of the system.
|
|
|
|
LAST_IMAGE |
Syntax of this supercard is the following:
LAST_IMAGE ... content of the supercard here ...
and the content is:
|
Card: ATOMIC_POSITIONS { alat | bohr | angstrom | crystal | crystal_sg } |
For the description of ATOMIC_POSITIONS card see file: INPUT_PW.html or INPUT_PW.txt
|
|
Card: TOTAL_CHARGE |
Optional card, needed only if lfcp == .TRUE.
Syntax:
TOTAL_CHARGE
|
Description of items:
tot_charge
|
REAL |
tot_charge is the total charge of the system.
|
|
|
|
|
END_POSITIONS |
Here can follow other pw specific cards ...
|
END_ENGINE_INPUT |
|
END |
|