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Re: about DDB file


Chronological Thread 
  • From: "D. R. Hamann" <drh@bell-labs.com>
  • To: Chun Li <chun.li@mf.mpg.de>, abinit_forum <forum@abinit.org>
  • Subject: Re: about DDB file
  • Date: Thu, 28 Oct 2004 12:32:06 -0400

Dear Chun,

Please send your Abinit questions to the forum rather than my personal
email.

I think your anaddb issue relates to your first run being cut off.  Abinit
only writes the DDB file after in completes all the perturbations in
a given dataset, so I believe that is why part was missing.  You can
divide perturbations among different datasets, or even among different
runs and use the mrgddb utility.

There is a more serious issue.  If I am interpreting your data correctly,
it looks as if you have set up a slab surface model of ZnO with a vacuum
region.  The elastic tensor and piezoelectric tensor are bulk properties,
and are meaningless for such a model.

D. R. Hamann

Chun Li wrote:
Dear Hamann,

When I calculate the dielectric and piezoelectric tensor of wurtzite
structures using abinit, I encountered some problems.

1) When I perform such calculations on my supercell model, the
calculation cannot complete in the limited time of the machine. So I
restart the calculation by reading from the output WF files. That is,
read *_WFK and *_1WF13~15 obtained from the first two datasets. And for
the third dataset, I only calculate the perturbations that have not been
completed in the previous calculation. Is it right?

2) After the restart calculation completed, I used anaddb to analyze the
DDB file, but the result can not be obtained with some COMMENT like:
gtblk9 : COMMENT -
  The blok     1 does not match the requirement
  because it lacks the element with
  idir1,ipert1,idir2,ipert2,index=    1    1    1    1    1

and the following bug in the end of the log file:
matrginv : BUG -
  The matrix that has been passed in argument of this subroutine
  is probably either singular or nearly singular.
  Action : contact ABINIT group.

 Delivered    0 WARNINGs and  21 COMMENTs to log file.

I think this is relative to the restart calculation. But if the method I
used to restart the calculation is incorrect, then how to do it? Can you
give me some ideas? Thanks a lot.

The input file:
  ndtset  3

   iscf1  3
 kptopt1  1
 tolvrs1  1.0d-18 

   iscf2 -3
 rfelfd2  2
 getwfk2  -1
   nqpt2  1
    qpt2  0.0 0.0 0.0
 kptopt2  2
#getden2  1
  rfdir2  1 1 1
 tolwfr2  1.0d-20

 rfphon3  1
rfatpol3  1 4
   iscf3  3     
 rfelfd3  3 
   nqpt3  1
    qpt3  0.0 0.0 0.0   
 getwfk3  -2     
 getddk3  -1
  rfdir3  1 1 1
 rfstrs3  3
 kptopt3  2
 tolvrs3  1.0d-10

# Common data
  acell  6.15956186 18.47868558 12.16199678
  diemac  9.0
  diemix  0.1
    ecut  56.0
    iscf  3
   natom  4 
   nband  24
   ngkpt  6 2 2
  nloalg  4
 nshiftk  1
   nstep  500
  ntypat  2
  prtvol  10
  angdeg  90 90 120
  shiftk  0.0 0.0 0.5
    xred
0.0 0.0 0.0000000000
2/3 1/9 0.0954692557
2/3 1/9 0.4045307443
0.0 0.0 0.5000000000
# tolwfr  1.d-12
   typat  1 2 1 2 
   znucl  8 30

After the first calculation, the dataset2 is completed, and then I
restart the calculation with only the dataset3. After second
calculation, the dataset3 have not completed (only the phonon
perturbation is completed), so I restart again with only rfreld and
rfstrs. Then the DDB file (attached) is obtained after the third
calculation is completed.

Then I use the following anaddb input file to analyze it:

!the flags
dieflag 3  !the frequency dependent dielectric tensor is calculated
elaflag  3  !the flag for the elastic constant
piezoflag 3
instrflag 1  !the flag for the internal strain tensor

!the effective charge part
asr 1
chneut  1

! Wavevector list number 1

nph1l 1 !number of phonons in list 1
qph1l  0.0 0.0 0.0 1.0 !the Gamma point

! Wave vector list no. 2

nph2l 1  !number of phonons in list 2
qph2l 0.0 0.0 1.0 0.0  ! why here the normalization factor is 0

Sorry for wasting your time. Any advice from you is appreciated. Thank
you again.

Best regards.

Chun Li
  

**** DERIVATIVE DATABASE **** +DDB, Version number 10929 Note : temporary (transfer) database natom 4 nkpt 12 nsppol 1 nsym 2 ntypat 2 occopt 1 nband 24 acell 0.61595618600000D+01 0.18478685580000D+02 0.12161996780000D+02 amu 0.15999400000000D+02 0.65390000000000D+02 dilatmx 0.10000000000000D+01 ecut 0.56000000000000D+02 ecutsm 0.00000000000000D+00 intxc 0 iscf 3 ixc 2 kpt 0.00000000000000D+00 0.00000000000000D+00 0.25000000000000D+00 0.16666666666667D+00 0.00000000000000D+00 0.25000000000000D+00 0.33333333333333D+00 0.00000000000000D+00 0.25000000000000D+00 0.50000000000000D+00 0.00000000000000D+00 0.25000000000000D+00 -0.33333333333333D+00 0.00000000000000D+00 0.25000000000000D+00 -0.16666666666667D+00 0.00000000000000D+00 0.25000000000000D+00 0.00000000000000D+00 0.50000000000000D+00 0.25000000000000D+00 0.16666666666667D+00 0.50000000000000D+00 0.25000000000000D+00 0.33333333333333D+00 0.50000000000000D+00 0.25000000000000D+00 0.50000000000000D+00 0.50000000000000D+00 0.25000000000000D+00 -0.33333333333333D+00 0.50000000000000D+00 0.25000000000000D+00 -0.16666666666667D+00 0.50000000000000D+00 0.25000000000000D+00 kptnrm 0.10000000000000D+01 ngfft 45 135 90 nspden 1 nspinor 1 occ 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.20000000000000D+01 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 rprim 0.10000000000000D+01 0.00000000000000D+00 0.00000000000000D+00 -0.50000000000000D+00 0.86602540378444D+00 0.00000000000000D+00 0.61232339957368D-16 0.10605752387249D-15 0.10000000000000D+01 sciss 0.00000000000000D+00 spinat 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 symafm 1 1 symrel 1 0 0 0 1 0 0 0 1 -1 0 0 3 1 0 0 0 1 tnons 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 tolwfr 0.10000000000000D+01 tphysel 0.00000000000000D+00 tsmear 0.40000000000000D-01 typat 1 2 1 2 wtk 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 0.83333333333333D-01 xred 0.00000000000000D+00 0.00000000000000D+00 0.00000000000000D+00 0.66666666666667D+00 0.11111111111111D+00 0.95469255700000D-01 0.66666666666667D+00 0.11111111111111D+00 0.40453074430000D+00 0.25431029499041D-32 0.16954019666027D-32 0.50000000000000D+00 znucl 0.80000000000000D+01 0.30000000000000D+02 zion 0.60000000000000D+01 0.12000000000000D+02 Description of the potentials (KB energies) vrsio8 (for pseudopotentials)= 10929 dimekb = 3 lmnmax= 3 usepaw= 0 Atom type= 1 pspso= 1 nekb= 1 iln lpsang iproj ekb(:) 1 1 1 -4.6233336E+00 Atom type= 2 pspso= 1 nekb= 2 iln lpsang iproj ekb(:) 1 1 1 3.4796927E+01 0.0000000E+00 2 2 1 0.0000000E+00 -1.3650335E+01 **** Database of total energy derivatives **** Number of data blocks= 1 2rd derivatives (non-stat.) - # elements : 239 qpt 0.00000000E+00 0.00000000E+00 0.00000000E+00 1.0 1 1 3 1 0.00000000000000D+00 0.00000000000000D+00 1 1 3 2 0.00000000000000D+00 0.00000000000000D+00 1 1 3 3 0.00000000000000D+00 0.00000000000000D+00 1 1 3 4 0.00000000000000D+00 0.00000000000000D+00 1 1 1 6 -0.50859795675800D+02 0.00000000000000D+00 1 1 2 6 -0.10080031888440D-12 0.00000000000000D+00 1 1 3 6 -0.69302569371436D-13 0.00000000000000D+00 1 1 1 7 -0.45702385318229D-13 0.00000000000000D+00 1 1 2 7 0.56025935368386D-14 0.00000000000000D+00 1 1 3 7 -0.24107819435486D-14 0.00000000000000D+00 1 1 1 8 -0.69151598822178D-14 0.00000000000000D+00 1 1 2 8 -0.68421752719346D+00 0.00000000000000D+00 1 1 3 8 -0.91302803396521D+00 0.00000000000000D+00 2 1 1 6 0.14895597965130D+02 0.00000000000000D+00 2 1 2 6 -0.40929396867052D+02 0.00000000000000D+00 2 1 3 6 -0.52461977224748D+01 0.00000000000000D+00 2 1 1 7 -0.16922857561349D+01 0.00000000000000D+00 2 1 2 7 -0.16882700819234D+01 0.00000000000000D+00 2 1 3 7 -0.13940933022715D+01 0.00000000000000D+00 2 1 1 8 -0.45143867200671D+00 0.00000000000000D+00 2 1 2 8 0.10263262907912D+01 0.00000000000000D+00 2 1 3 8 0.13695420509378D+01 0.00000000000000D+00 3 1 1 1 0.00000000000000D+00 0.00000000000000D+00 3 1 1 2 0.00000000000000D+00 0.00000000000000D+00 3 1 1 3 0.00000000000000D+00 0.00000000000000D+00 3 1 1 4 0.00000000000000D+00 0.00000000000000D+00 3 1 1 6 -0.78199504690861D-01 0.00000000000000D+00 3 1 2 6 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0.22080947084563D-01 0.00000000000000D+00 1 8 1 8 0.32420536556469D+00 0.00000000000000D+00 1 8 2 8 -0.10568851162750D-10 0.00000000000000D+00 1 8 3 8 0.78682654425545D-11 0.00000000000000D+00 2 8 1 7 0.18903890235407D-13 0.00000000000000D+00 2 8 2 7 -0.14837148907551D-13 0.00000000000000D+00 2 8 3 7 -0.27810497980504D-13 0.00000000000000D+00 2 8 1 8 -0.12186513089677D-13 0.00000000000000D+00 2 8 2 8 0.61039079201925D+00 0.00000000000000D+00 2 8 3 8 0.42664136399872D-01 0.00000000000000D+00 3 8 1 7 0.35067795162272D-13 0.00000000000000D+00 3 8 2 7 -0.20714050046926D-12 0.00000000000000D+00 3 8 3 7 -0.65747670591335D-13 0.00000000000000D+00 3 8 1 8 -0.12864976884352D-13 0.00000000000000D+00 3 8 2 8 0.42664140999881D-01 0.00000000000000D+00 3 8 3 8 0.54694519809311D+00 0.00000000000000D+00

-- 
D. R. Hamann				Phone: 908-582-4454
Director, Theoretical Materials    	Fax:   908-582-4702
  Physics Research (retired)		email: drh@physics.bell-labs.com
Bell Laboratories 
Lucent Technologies
700 Mountain Ave, Room 1D-371
Murray Hill, NJ 07974-0636 USA



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