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Re: [abinit-forum] Definition of hexagonal unit


Chronological Thread 
  • From: Xavier Gonze <gonze@pcpm.ucl.ac.be>
  • To: forum@abinit.org
  • Subject: Re: [abinit-forum] Definition of hexagonal unit
  • Date: Mon, 6 Feb 2006 10:55:27 +0100

Dear Tanaka Yoshikazu,

At least two input variables have questionable values :
- ecut 6 is likely much too low (for Vanadium, I guess you need at least 25 - remember convergence studies are up to the user)
- toldfe 1.0d-6 is likely too large for converged forces, and the use of toldfe is not recommended for structural optimization.
Use toldff or tolvrs instead, e.g. with a value toldff 1.0d-6

May be there are other problems ...
Xavier

On 06 Feb 2006, at 04:40, Tanaka Yoshikazu wrote:

Dear Xavier,

Thank you very much for your kind reply.

I am studing on phonons in BaVS3, which has hexagonal structure (a=6.74, c=5.61
angstroms) at room temperature. This is a metal at room temperature, and
insulator below 70 K with orthorhombic structure.
I took the crystal structure from "Acta Cryst. B25 781 (1969).

First, I tried to calculate the total energy with the following
input file.

The result shows unusual forces among atoms 3,4,5 and 8,9,10.
(S atoms have strong forces each other.)
Does this means that the real existing crystal
in hexagonal structure is unstable?

Once I tried
#Optimization of the lattice parameters
optcell 2
ionmov 3
ntime 10
dilatmx 1.1
ecutsm 0.5
but, the calculation did not complete becasue dilatmx 1.1 is not enough.

With regards,
Yoshikazu

cartesian forces (hartree/bohr) at end:
1 0.00000000000000 0.00000000000000 0.00000000000000
2 0.00000000000000 0.00000000000000 0.00000000000000
3 0.00000000000000 0.04802739569869 0.00000000000000
4 -0.04159294475268 -0.02401369784935 0.00000000000000
5 0.04159294475268 -0.02401369784935 0.00000000000000
6 0.00000000000000 0.00000000000000 0.00000000000000
7 0.00000000000000 0.00000000000000 0.00000000000000
8 0.00000000000000 -0.04802739569869 0.00000000000000
9 0.04159294475268 0.02401369784935 0.00000000000000
10 -0.04159294475268 0.02401369784935 0.00000000000000
frms,max,avg= 2.1478504E-02 4.8027396E-02 0.000E+00 0.000E+00 0.000E+00 h/b

Input file----------------------------------------------------------------
# Crystalline BaVS3 : computation of the total energy
#
occopt 4
tsmear 0.05
#Specific to ground state calculation
kptopt 1 # Automatic generation of k points, taking
# into account the symmetry
# tolvrs 1.0d-18 # SCF stopping criterion
iscf 5 # Self-consistent calculation, using algorithm 5

###################################################################### #
#Common input variables

#Definition of the unit cell
acell 6.724 6.724 5.610 angstrom
angdeg 90 90 120
spgroup 194
#rprim 1.0 0.0 0.0 # In lessons 1 and 2, these primitive vectors
# 0.0 1.0 0.0 # (to be scaled by acell) were 1 0 0 0 1 0 0 0 1
# 0.0 0.0 1.0 # that is, the default.

#Definition of the atom types
ntypat 3 # There are two types of atom
znucl 56 23 16 # 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, type 1 is the Aluminum,
# type 2 is the Arsenic.

#Definition of the atoms
natom 10 # There are two atoms
typat 1 2 3 3 3 1 2 3 3 3
xred # This keyword indicate that the location of the atoms
2/3 1/3 1/4
0.0 0.0 0.0
0.1656 0.3312 0.25
0.6688 0.8344 0.25
0.1656 0.8344 0.25
1/3 2/3 3/4
0.0 0.0 1/2
0.8344 0.6688 0.75
0.3312 0.1656 0.75
0.8344 0.1656 0.75

#Exchange-correlation functional
ixc 1 # LDA Teter Pade parametrization

#Definition of the planewave basis set
ecut 6.0 # Maximal kinetic energy cut-off, in Hartree

#Definition of the k-point grid
ngkpt 4 4 4
nshiftk 1
shiftk 0.0 0.0 0.5

#Definition of the SCF procedure
nstep 35 # Maximal number of SCF cycles
toldfe 1.0d-6

With regards,
Yoshikazu
--
Tanaka Yoshikazu, SPring-8/RIKEN
Mikazuki, Sayo, Hyogo 679-5148,
Portable Phone +81-7915-8-0802-0-3347,
Fax +81-7915-8-2923
email ytanaka@postman.riken.jp





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