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- From: gf98lfl@geo.geol.ku.dk
- To: forum@abinit.org
- Subject: Adding pressure in steps of 2GPA
- Date: Fri, 18 Jul 2003 12:51:46 +0200
Hi ABINIT users.
I am calculating the effect of pressure on the structure of bismuthinite. To
calculate the structure at a series of pressure I use the commands getcell,
getxred with ndtset (see inputfile at the end of this message).
The first dataset is running fine but there is a problem when it is starting
dataset 2.
This memory test is taken from the beginning of the log file:
DATASET 2 : space group Pn m a (# 62); Bravais oP (primitive ortho.)
================================================================================
Values of the parameters that define the memory need for DATASET 2.
intxc = 0 ionmov = 2 iscf = 5 ixc =
1
lmnmax = 2 lnmax = 2 mband = 59 mffmem =
1
mgfft = 64 mkmem = 1 mpssoang= 3 mpw =
4868
mqgrid = 1201 natom = 20 nfft = 98304 nkpt =
1
nloalg = 4 nspden = 1 nspinor = 1 nsppol =
1
nsym = 8 n1xccc = 2501 ntype = 2 occopt =
1
================================================================================
memory : COMMENT -
The determination of memory needs at this stage is meaningless,
since getcell = -1 is non-zero, while idtset= 2.
The following numbers are obtained by supposing that acell and rprim
are NOT taken from a previous dataset. You cannot rely on them.
This job should need less than 27.621 Mbytes of memory.
Rough estimation (10% accuracy) of disk space for files :
WF disk file : 4.385 Mbytes ; DEN or POT disk file : 0.752 Mbytes.
================================================================================
It comments that the determination of memory needs at this stage is
meaningless. When it is starting the calculations of dataset 2 it is doing
new memory test based on the new unit cell parameters and atom positions and
it finds a different mpw value from the one calculated above, and it stops
the calculations.
This is from the end of the log file:
== DATASET 2
==================================================================
mkfilename : getwfk/=0, take file _WFK from output of DATASET 1.
driver : getcell/=0, take acell and rprim from output of dataset with index
1.
driver : getxred/=0, take xred from output of dataset with index 1.
iofn2 : deduce lmnmax = 8, lnmax = 2,
lmnmaxso= 8, lnmaxso= 2.
Unit cell volume ucvol= 3.2276485E+03 bohr^3
Angles (23,13,12)= 9.00000000E+01 9.00000000E+01 9.00000000E+01 degrees
getcut: wavevector= 0.0000 0.0000 0.0000 ngfft= 64 24 64
ecut(hartree)= 10.000 => boxcut(ratio)= 2.10575
kpgsph : BUG -
npw= 4875 > mpw= 4868.
Action : contact ABINIT group.
Delivered 3 WARNINGs and 25 COMMENTs to log file.
leave_new : decision taken to exit ...
FORTRAN STOP 1
Is this a bug or am I doing something wrong ??
I am using ABINIT_4.0.2 on a pc using Linux.
Best regards
Lars Lundegaard
Inputfile:
# Bismuthinite (Bi2S3) crystal in pressure range 0-50 GPa in steps of 2 GPa.
prtden 1
getwfk -1
getcell -1
getxred -1
ndtset 26
#Structure optimization
optcell 2
ionmov 2
ntime 50
ecutsm 1.0
tolmxf 5.0E-04
strtarget1 0.0 0.0 0.0 0.0
0.0 0.0
strtarget2 -0.0000679785784542 -0.0000679785784542 -0.0000679785784542 0.0
0.0 0.0
strtarget3 -0.0001359571569084 -0.0001359571569084 -0.0001359571569084 0.0
0.0 0.0
strtarget4 -0.0002039357353626 -0.0002039357353626 -0.0002039357353626 0.0
0.0 0.0
strtarget5 -0.0002719143138168 -0.0002719143138168 -0.0002719143138168 0.0
0.0 0.0
strtarget6 -0.0003398928922710 -0.0003398928922710 -0.0003398928922710 0.0
0.0 0.0
strtarget7 -0.0004078714707252 -0.0004078714707252 -0.0004078714707252 0.0
0.0 0.0
strtarget8 -0.0004758500491794 -0.0004758500491794 -0.0004758500491794 0.0
0.0 0.0
strtarget9 -0.0005438286276336 -0.0005438286276336 -0.0005438286276336 0.0
0.0 0.0
strtarget10 -0.0006118072060878 -0.0006118072060878 -0.0006118072060878 0.0
0.0 0.0
strtarget11 -0.0006797857845420 -0.0006797857845420 -0.0006797857845420 0.0
0.0 0.0
strtarget12 -0.0007477643629962 -0.0007477643629962 -0.0007477643629962 0.0
0.0 0.0
strtarget13 -0.0008157429414504 -0.0008157429414504 -0.0008157429414504 0.0
0.0 0.0
strtarget14 -0.0008837215199046 -0.0008837215199046 -0.0008837215199046 0.0
0.0 0.0
strtarget15 -0.0009517000983588 -0.0009517000983588 -0.0009517000983588 0.0
0.0 0.0
strtarget16 -0.0010196786768130 -0.0010196786768130 -0.0010196786768130 0.0
0.0 0.0
strtarget17 -0.0010876572552672 -0.0010876572552672 -0.0010876572552672 0.0
0.0 0.0
strtarget18 -0.0011556358337214 -0.0011556358337214 -0.0011556358337214 0.0
0.0 0.0
strtarget19 -0.0012236144121756 -0.0012236144121756 -0.0012236144121756 0.0
0.0 0.0
strtarget20 -0.0012915929906298 -0.0012915929906298 -0.0012915929906298 0.0
0.0 0.0
strtarget21 -0.0013595715690840 -0.0013595715690840 -0.0013595715690840 0.0
0.0 0.0
strtarget22 -0.0014275501475382 -0.0014275501475382 -0.0014275501475382 0.0
0.0 0.0
strtarget23 -0.0014955287259924 -0.0014955287259924 -0.0014955287259924 0.0
0.0 0.0
strtarget24 -0.0015635073044466 -0.0015635073044466 -0.0015635073044466 0.0
0.0 0.0
strtarget25 -0.0016314858829008 -0.0016314858829008 -0.0016314858829008 0.0
0.0 0.0
strtarget26 -0.0016994644613550 -0.0016994644613550 -0.0016994644613550 0.0
0.0 0.0
#Definition of the unit cell
acell 11.292589298917 3.784531757523 11.174608388697 angstroms
angdeg 90 90 90
#Definition of the atom types
ntype 2 # There is only two types of atoms
znucl 16 83 # 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.
#Space group
spgroup 62
#Definition of the atoms
natom 20
type 1 1 1 2 2 1 1 1 2 2 1 1 1 2 2 1 1 1 2 2
xred
4.9193925706E-02 2.5000000000E-01 1.2956009361E-01
3.7483036124E-01 2.5000000000E-01 5.1935240141E-02
2.2129874293E-01 2.5000000000E-01 8.0396597496E-01
8.7512403610E-03 2.5000000000E-01 6.7684353662E-01
3.3216974466E-01 2.5000000000E-01 4.7127573578E-01
5.4919392571E-01 2.5000000000E-01 3.7043990639E-01
8.7483036124E-01 2.5000000000E-01 4.4806475986E-01
7.2129874293E-01 2.5000000000E-01 6.9603402504E-01
5.0875124036E-01 2.5000000000E-01 8.2315646338E-01
8.3216974466E-01 2.5000000000E-01 2.8724264219E-02
4.5080607429E-01 7.5000000000E-01 6.2956009361E-01
1.2516963876E-01 7.5000000000E-01 5.5193524014E-01
2.7870125707E-01 7.5000000000E-01 3.0396597496E-01
4.9124875964E-01 7.5000000000E-01 1.7684353662E-01
1.6783025534E-01 7.5000000000E-01 9.7127573578E-01
9.5080607429E-01 7.5000000000E-01 8.7043990639E-01
6.2516963876E-01 7.5000000000E-01 9.4806475986E-01
7.7870125707E-01 7.5000000000E-01 1.9603402504E-01
9.9124875964E-01 7.5000000000E-01 3.2315646338E-01
6.6783025534E-01 7.5000000000E-01 5.2872426422E-01
#Definition of the planewave basis set
ecut 10.0 # Maximal plane-wave kinetic energy cut-off, in Hartree
#Definition of the k-point grid
kptopt 1
ngkpt 2 2 2
#Definition of the SCF procedure
nstep 30 # Maximal number of SCF cycles
toldfe 1.0d-6 # Will stop when, twice in a row, the difference
# between two consecutive evaluations of total energy
# differ by less than toldfe (in Hartree)
diemac 1.0 # Although this is not mandatory, it is worth to
# precondition the SCF cycle. The model dielectric
diemix 0.5 # function used as the standard preconditioner
# is described in the "dielng" input variable section.
- Adding pressure in steps of 2GPA, gf98lfl, 07/18/2003
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