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IFC code and the phonon fequency of a material with hcp-structure?


Chronological Thread 
  • From: "Kwan-Woo Lee" <kwlee@ucdavis.edu>
  • To: forum@abinit.org
  • Subject: IFC code and the phonon fequency of a material with hcp-structure?
  • Date: Mon, 16 Sep 2002 22:09:27 -0700 (PDT)

Dear ABINIT Users,

I have a few questions. Could you help me?

1) Did you use the ifc-code in order to obtain a phonon dispersion
relation?
I don't exactly understand the required step.
First, obtain the DDB files using ABINIT main code at a few symmetry
points.
Second, merge the DDB files using mrgddb code.
Third, obtain the final results using ifc code.

Is the step correct ?


2) Is there one that have ever tried to obtain the phonon frequency, with
hcp-structure, contained E-field perturbation?
I obtained it of several materials with the fcc structure, however I have
not solved the problem
of hcp-structure. This is a input file (also attached) of LiB with
hcp-structure. (For non-E field perturbation, I obtained the phonon
frequencies)

###########################################################################
ndtset 3

# Specific to ground state calculation
kptopt1 1 #1,2 or 3
mkmem1 0
tolvrs1 1.0d-18
iscf1 5

# Response Function calculation : d/dk
rfelfd2 2
rfdir2 1 0 0 # In the x-direction.

nqpt2 1
qpt2 0.0 0.0 0.0 # For a Gamma point

getwfk2 -1
kptopt2 2

iscf2 -3
tolwfr2 1.0d-22

# To calculate RF, with q=0: E-field perturbation
rfphon3 1
rfatpol3 1 4
rfelfd3 3 # only the generation of the first-order
response
# to the electric field
rfdir3 1 1 1
kptopt3 2

nqpt3 1
qpt3 0.0 0.0 0.0 # Gamma point

getwfk3 -2 # Read the previous result(groundstate Cal.)
getddk3 -1 # Using the ouput of the dataset2

tolvrs3 1.0d-10
iscf3 5

######################################################Common Input
variables
#Definition of the unit cell
acell 2*4.022 2.796 angstrom

rprim 0.86602540378 0.500 0.000 # Primitive vectors
-0.86602540378 0.500 0.000
0.000 0.000 1.000

#spgroup 194 # the number of space group
# brvltt 1 # from the table
chkprim 0
occopt 4
ntype 2 # There are only three types of atom
zatnum 3 5 # The keyword "zatnum" refers to the atomic number of
the
# possible type(s) of atom.

#Definition of the atoms
natom 4 # There are four atoms
type 2 2 1 1 #
xred
0.00 0.00 0.00 # Triplet giving the reduced coordinates of atom 1, in
Bohr
0.00 0.00 0.50
0.6666666666666666667 0.3333333333333333333 0.00 # of atom 2, in Bohr
0.3333333333333333333 0.6666666666666666667 0.50

#Definition of the planewave basis set
#ecut 10.0 # Maximal plane-wave kinetic energy cut-off, in Hartree
ecut 5.0
dilatmx 1.10

# Gives the number of band
nband 8 # Not determined.

#Definition of the k-point grid( afther testing, determined.)
#prtkpt 1 # to genertate "kptrlatt" and "shiftk"
kptrlatt 2 0 0
0 2 0
0 0 3
nshiftk 1
shiftk 0.00000000 0.00000000 5.00000000E-01

#Definition of the SCF procedure
nstep 40 # Maximal number of SCF cycles

###########################################################################

If you have any hint, please let me know it.
I will very apprecite for it.

Sincerely,

Kwan-Woo Lee

Attachment: lib_hcp.in
Description: lib_hcp.in




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