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- From: Shaorui Sun <sunsr@ihep.ac.cn>
- To: "forum@abinit.org" <forum@abinit.org>
- Subject: a question about the phonon computation
- Date: Wed, 18 May 2005 14:31:46 +0800
Dear all:
When I calculate the phonon mode of Ge,my result is different from the
experimental result which is shown in the follow table.
experimental(cm-1) computational(cm-1)
Gamma(TO) 304 289
Gamma(LO) 304 289
X(TA) 80 78
X(LA) 241 226
X(TO) 276 251
X(LO) 241 226
L(TA) 63 62
L(LA) 222 215
L(TO) 290 271
L(LO) 245 220
--------------------------------------------------------
It also looks like that the difference is more obvious with higher
frequency.My inout is shown as follows:
-----------------------------------------------------------------------
ndtset 6
#Definition of the k-point grids
kptopt 1 # Option for the automatic generation of k points, taking
# into account the symmetry
nshiftk 4
shiftk 0.5 0.5 0.5 # These shifts will be the same for all grids
0.5 0.0 0.0
0.0 0.5 0.0
0.0 0.0 0.5
ngkpt 8 8 8 # Definition of the different grids
#Ground state calculation
kptopt1 1 # Automatic generation of k po
# into account the symmetry
tolvrs1 1.0d-18 # SCF stopping criterion
iscf1 5 # Self-consistent calculation,
prtden1 1 # Will be needed for dataset 4
#Response Function calculation : phonon at X
rfphon2 1 # Activate the calculation of the atomic dispace
rfatpol2 1 1 # All the atoms will be displaced
rfdir2 1 1 1 # Need to consider the perturbation in the x-dir
nqpt2 1
qpt2 0.0 0.5 0.5 # This is a calculation at the X point
getwfk2 1 # Uses as input wfs the output wfs of the datase
kptopt2 3 # Automatic generation of k points,
# no use of symmetries to decrease
# the size of the k point set.
tolvrs2 1.0d-8
iscf2 5 # Self-consistent calculation, using algorithm 5
#Response Function calculation : phonon at L
rfphon3 1 # Activate the calculation of the atomic dispace
rfatpol3 1 1 # All the atoms will be displaced
rfdir3 1 1 1 # Need to consider the perturbation in the x-dir
nqpt3 1
qpt3 0.5 0.0 0.0 # This is a calculation at the L point
getwfk3 1 # Uses as input wfs the output wfs of the datase
kptopt3 3 # Automatic generation of k points,
# no use of symmetries to decrease
# the size of the k point set.
tolvrs3 1.0d-8
iscf3 5 # Self-consistent calculation, using algorithm 5
#Response Function calculation : phonon at Gamma
rfphon4 1 # Activate the calculation of the atomic
dispacement p
erturbations
rfatpol4 1 1 # All the atoms will be displaced
rfdir4 1 1 1 # Need to consider the perturbation in the
x-direction
only
nqpt4 1
qpt4 0.0 0.0 0.0 # This is a calculation at the Gamma point
getwfk4 1 # Uses as input wfs the output wfs of the dataset 1
kptopt4 2 # Automatic generation of k points,
# using only the time-reversal symmetry to decrease
# the size of the k point set.
tolvrs4 1.0d-8
iscf4 5 # Self-consistent calculation, using algorithm
#Response Function calculation : phonon at K
rfphon5 1 # Activate the calculation of the atomic
dispacement p
erturbations
rfatpol5 1 1 # All the atoms will be displaced
rfdir5 1 1 1 # Need to consider the perturbation in the
x-direction
only
nqpt5 1
qpt5 3/8 3/8 1/2 # This is a calculation at the Gamma point
getwfk5 1 # Uses as input wfs the output wfs of the dataset 1
kptopt5 3 # Automatic generation of k points,
# using only the time-reversal symmetry to decrease
# the size of the k point set.
tolvrs5 1.0d-8
iscf5 5 # Self-consistent calculation, using algorithm
#Response Function calculation : phonon at W
rfphon6 1 # Activate the calculation of the atomic
dispacement p
erturbations
rfatpol6 1 1 # All the atoms will be displaced
rfdir6 1 1 1 # Need to consider the perturbation in the
x-direction
only
nqpt6 1
qpt6 0.25 0.25 0.75 # This is a calculation at the Gamma point
getwfk6 1 # Uses as input wfs the output wfs of the dataset 1
kptopt6 3 # Automatic generation of k points,
# using only the time-reversal symmetry to decrease
# the size of the k point set.
tolvrs6 1.0d-8
iscf6 5 # Self-consistent calculation, using algorithm
#Definition of the unit cell
acell 3*10.68 # This is equivalent to 10.18 10.18 10.18
rprim 0.0 0.5 0.5 # FCC primitive vectors (to be scaled by acell)
0.5 0.0 0.5
0.5 0.5 0.0
#Definition of the atom types
ntypat 1 # There is only one type of atom
znucl 32 # The keyword "znucl" refers to the atomic number of the
# possible type(s) of atom. The pseudopotential(s)
# mentioned in the "files" file must correspond
# to the type(s) of atom. Here, the only type is Silicon.
#Definition of the atoms
natom 2 # There are two atoms
typat 1 1 # They both are of type 1, that is, Silicon.
xred # This keyword indicate that the location of the atoms
# will follow, one triplet of number for each atom
0.0 0.0 0.0 # Triplet giving the REDUCED coordinate of atom 1.
1/4 1/4 1/4 # Triplet giving the REDUCED coordinate of atom 2.
#Definition of the planewave basis set
ecut 8.0 # Maximal kinetic energy cut-off, in Hartree
#Definition of the SCF procedure
nstep 20 # Maximal number of SCF cycles
diemac 13.0 # Although this is not mandatory, it is worth to
# precondition the SCF cycle. The model dielectric
# function used as the standard preconditioner
# is described in the "dielng" input variable section.
# Here, we follow the prescription for bulk silicon.
[wien2k@bsrf-serv temp]$ vi Ge.in
#Crystalline silicon : computation of the total energy
# Convergence with respect to the number of k points.
ndtset 6
#Definition of the k-point grids
kptopt 1 # Option for the automatic generation of k points, taking
# into account the symmetry
nshiftk 4
shiftk 0.5 0.5 0.5 # These shifts will be the same for all grids
0.5 0.0 0.0
0.0 0.5 0.0
0.0 0.0 0.5
ngkpt 8 8 8 # Definition of the different grids
#Ground state calculation
kptopt1 1 # Automatic generation of k po
# into account the symmetry
tolvrs1 1.0d-18 # SCF stopping criterion
iscf1 5 # Self-consistent calculation,
prtden1 1 # Will be needed for dataset 4
#Response Function calculation : phonon at X
rfphon2 1 # Activate the calculation of the atomic dispace
rfatpol2 1 1 # All the atoms will be displaced
rfdir2 1 1 1 # Need to consider the perturbation in the x-dir
nqpt2 1
qpt2 0.0 0.5 0.5 # This is a calculation at the X point
getwfk2 1 # Uses as input wfs the output wfs of the datase
kptopt2 3 # Automatic generation of k points,
# no use of symmetries to decrease
# the size of the k point set.
tolvrs2 1.0d-8
iscf2 5 # Self-consistent calculation, using algorithm 5
#Response Function calculation : phonon at L
rfphon3 1 # Activate the calculation of the atomic dispace
rfatpol3 1 1 # All the atoms will be displaced
rfdir3 1 1 1 # Need to consider the perturbation in the x-dir
nqpt3 1
qpt3 0.5 0.0 0.0 # This is a calculation at the L point
getwfk3 1 # Uses as input wfs the output wfs of the datase
kptopt3 3 # Automatic generation of k points,
# no use of symmetries to decrease
# the size of the k point set.
tolvrs3 1.0d-8
iscf3 5 # Self-consistent calculation, using algorithm 5
#Response Function calculation : phonon at Gamma
rfphon4 1 # Activate the calculation of the atomic
dispacement p
erturbations
rfatpol4 1 1 # All the atoms will be displaced
rfdir4 1 1 1 # Need to consider the perturbation in the
x-direction
only
nqpt4 1
qpt4 0.0 0.0 0.0 # This is a calculation at the Gamma point
getwfk4 1 # Uses as input wfs the output wfs of the dataset 1
kptopt4 2 # Automatic generation of k points,
# using only the time-reversal symmetry to decrease
# the size of the k point set.
tolvrs4 1.0d-8
iscf4 5 # Self-consistent calculation, using algorithm
#Response Function calculation : phonon at K
rfphon5 1 # Activate the calculation of the atomic
dispacement p
erturbations
rfatpol5 1 1 # All the atoms will be displaced
rfdir5 1 1 1 # Need to consider the perturbation in the
x-direction
only
nqpt5 1
qpt5 3/8 3/8 1/2 # This is a calculation at the Gamma point
getwfk5 1 # Uses as input wfs the output wfs of the dataset 1
kptopt5 3 # Automatic generation of k points,
# using only the time-reversal symmetry to decrease
# the size of the k point set.
tolvrs5 1.0d-8
iscf5 5 # Self-consistent calculation, using algorithm
#Response Function calculation : phonon at W
rfphon6 1 # Activate the calculation of the atomic
dispacement p
erturbations
rfatpol6 1 1 # All the atoms will be displaced
rfdir6 1 1 1 # Need to consider the perturbation in the
x-direction
only
nqpt6 1
qpt6 0.25 0.25 0.75 # This is a calculation at the Gamma point
getwfk6 1 # Uses as input wfs the output wfs of the dataset 1
kptopt6 3 # Automatic generation of k points,
# using only the time-reversal symmetry to decrease
# the size of the k point set.
tolvrs6 1.0d-8
iscf6 5 # Self-consistent calculation, using algorithm
#Definition of the unit cell
acell 3*10.68
rprim 0.0 0.5 0.5 # FCC primitive vectors (to be scaled by acell)
0.5 0.0 0.5
0.5 0.5 0.0
#Definition of the atom types
ntypat 1 # There is only one type of atom
znucl 32 # The keyword "znucl" refers to the atomic number of the
# possible type(s) of atom. The pseudopotential(s)
# mentioned in the "files" file must correspond
# to the type(s) of atom. Here, the only type is Silicon.
#Definition of the atoms
natom 2 # There are two atoms
typat 1 1 # They both are of type 1, that is, Silicon.
xred # This keyword indicate that the location of the atoms
# will follow, one triplet of number for each atom
0.0 0.0 0.0 # Triplet giving the REDUCED coordinate of atom 1.
1/4 1/4 1/4 # Triplet giving the REDUCED coordinate of atom 2.
#Definition of the planewave basis set
ecut 8.0 # Maximal kinetic energy cut-off, in Hartree
#Definition of the SCF procedure
nstep 20 # Maximal number of SCF cycles
diemac 13.0 # Although this is not mandatory, it is worth to
# precondition the SCF cycle. The model dielectric
# function used as the standard preconditioner
# is described in the "dielng" input variable section.
# Here, we follow the prescription for bulk silicon.
----------------------------------------------------------------------
Who could give me some suggestion or direction?
Thanks in advance!
Best Regards!
S. R. Sun
---------------------------------------------
Beijing Synchrotron Radiation Facility
Institute of High Energy Physics
Chinese Academy of Sciences
P. O. Box 918, 100049 Beijing
P. R. China
Tel: 0086+10 88236710
email:sunsr@ihep.ac.cn
- a question about the phonon computation, Shaorui Sun, 05/18/2005
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