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- From: m-takahashi@hq.jp.nec.com
- To: forum@abinit.org
- Subject: Re: Re: Re: [abinit-forum] On the latticed optimization
- Date: Thu, 25 Nov 2004 16:07:16 +0900
Dear Yukihiro Okuno and ABINIT users
I think "occopt" option is needed for smearing of occupation numbers.
I modified your input file as follows;
---------------------------------------------------------
#Definition of the unit cell
optcell 1
ionmov 2
ntime 20
dilatmx 1.05 #changed
prtwf 0
prtden 1
acell 10.0 10.0 10.0
rprim 0.000000000000 0.5 0.5
0.5 0.000000000000 0.5
0.5 0.5 0.000000000000
ntypat 1
znucl 82
natom 1
typat 1
xcart
0.000000000000 0.000000000000 0.000000000000
nband 12 #changed
occopt 7 #changed
tsmear 0.04
kptopt 1
ngkpt 8 8 8
ecut 40 # 1088 eV
ecutsm 0.5 #changed
ixc 3
nstep 20
toldfe 1.0d-5 eV #changed
tolmxf 0.001 #changed
#toldff 1.0d-7
diemac 12.0
------------------------------------------------------
I obtained converged acell value of 9.3142013293E+00 bohr
using Teter extended norm-conserving PP (available on ABINIT web site)
with ABINIT v.4.2.3 for Windows.
sincerely.
Masatake Takahashi
>
>I'm now testing the calculation of fcc-lattice
>of the Pb for lattice optimization.
>
>I use Teter's extended norm-conserving pseudo
>potential which I downloaded from the ABINIT site.
>
>The results and calculation depends on the initial
>guess of acell or scaling of relation of the acell
>and rprim.
>
>On the initial acell,
>
> I had first sets acell = 9.3548995339E+00 ( corresponds
> latticd constant of the fcc cube), the calculation of
> the results failed with the massage
> BROYDEN STEP NUMBER 3
> ------------------------------------------------------
>
> metric : ERROR -
> Current rprimd gives negative (R1xR2).R3 .
> Rprimd = 0.000000E+00 -1.073389E-01 -1.073389E-01
> -1.073389E-01 0.000000E+00 -1.073389E-01
> -1.073389E-01 -1.073389E-01 0.000000E+00
>
> and, if I set acell = 10.00 I can get the conversed
> results.
>
> But the conversed results is that acell = 1.0345762121E+01
> which is rather larger than the experimental vales,
> a = 9.353198. Basically is the origin of the discrepancy
> due to the pseudo-potential of lead ?
>
> And On the scaling relation of acell and rprim, I set
> acell = a/sqrt(2), and rprim = 0, 1/sqrt(2), 1/sqrt(2)
> ( for example), the calculation is also failed with the
> message, ( in this case I set rather small value of dilatmx)
>
>The new primitive vectors rprimd (an evolving quantity)
> are too large with respect to the old rprimd and the accompanying dilatmx :
> this large change of unit cell parameters is not allowed by the present
> value of dilatmx.
> You need at least dilatmx= 1.657208E+00)
>
> I use ABINIT-4.2.3 on the DOS/WIn-Intel-PGI version.
>
> Sincerely,
>
> Yukihir Okuno.
>
>
>The results of the lattice optimization of fcc-Pb crystal
>with Teter's pseudo potential. the experimental
>value of the lattice constant of fcc cube is 9.353198.
>
>-outvars: echo values of variables after computation --------
> acell 1.0345762121E+01 1.0345762121E+01 1.0345762121E+01 Bohr
> amu 2.07200000E+02
> diemac 1.20000000E+01
> dilatmx 2.00000000E+00
> ecut 4.00000000E+01 Hartree
> ecutsm 5.00000000E+00 Hartree
> etotal -5.9806901453E+01
> fcart 0.0000000000E+00 0.0000000000E+00 0.0000000000E+00
> ionmov 2
> ixc 3
>
>
>
>Here is my input file.
>
>#Definition of the unit cell
>optcell 1
>ionmov 2
>ntime 20
>dilatmx 2.0
>ptrwf 0
>
>acell 10.0 10.0 10.0
>
>rprim 0.000000000000 0.5 0.5
> 0.5 0.000000000000 0.5
> 0.5 0.5 0.000000000000
>
>ntypat 1
>znucl 82
>natom 1
>typat 1
>xcart
> 0.000000000000 0.000000000000 0.000000000000
>
>tsmear 0.04
>kptopt 1
>ngkpt 8 8 8
>ecut 40
>ecutsm 5.0
>ixc 3
>nstep 10
>toldff 1.0d-7
>diemac 12.0
----------------------------------
NEC Corp.
Masatake Takahashi
m-takahashi@hq.jp.nec.com
----------------------------------
- Re: Re: [abinit-forum] On the latticed optimization, yukihiro_okuno, 11/23/2004
- <Possible follow-up(s)>
- Re: Re: Re: [abinit-forum] On the latticed optimization, yukihiro_okuno, 11/25/2004
- Re: Re: Re: [abinit-forum] On the latticed optimization, m-takahashi, 11/25/2004
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