Hi!
I have tried to calculate the static dielectric constant e(0) with ionic contribution for rutile, using
LEPSILON = .TRUE.
LPEAD = .TRUE.
IBRION = 8
following the advice of the manual. Having no experience with this whatsoever, I specified NSW = 30. VASP finished after writing 30 F =... in the OSZICAR file (see below), and gave me some (reasonably good) values for e(0) in the OUTCAR file.
Now I have two questions:
1) How do I know, whether this is the convergent end result or not?
2) If it is not, can I just continue (with ISTART = 1) where it has been left off?
Thanks for any help.
Peter Deak
30 F= -.53573739E+02 E0= -.53573739E+02 d E =-.188484-190
Linear response reoptimize wavefunctions
DAV: 1 -0.535737387889E+02 -0.90949E-12 0.41252E-12 9600 0.147E-11
Linear response to external field (no local field effect), progress :
Direction: 1
N E dE d eps ncg rms rms(c)
RMM: 1 -0.935640519800E+00 -0.93564E+00 -0.42877E+00 4424 0.444E+00
RMM: 2 -0.118419483176E+01 -0.24855E+00 -0.15732E-02 4910 0.303E-01
RMM: 3 -0.118545515813E+01 -0.12603E-02 -0.32488E-04 4948 0.308E-02
RMM: 4 -0.118545556881E+01 -0.41068E-06 -0.15992E-06 4193 0.182E-03
Linear response to external field (no local field effect), progress :
Direction: 2
N E dE d eps ncg rms rms(c)
RMM: 1 -0.861118966524E+00 -0.86112E+00 -0.37369E+00 4423 0.446E+00
RMM: 2 -0.109300148717E+01 -0.23188E+00 -0.13644E-02 4901 0.302E-01
RMM: 3 -0.109445621172E+01 -0.14547E-02 -0.35517E-04 4950 0.319E-02
RMM: 4 -0.109445677703E+01 -0.56531E-06 -0.16460E-06 4204 0.185E-03
Linear response to external field (no local field effect), progress :
Direction: 3
N E dE d eps ncg rms rms(c)
RMM: 1 -0.110999745586E+01 -0.11100E+01 -0.49203E+00 4402 0.458E+00
RMM: 2 -0.136572120827E+01 -0.25572E+00 -0.18867E-02 4918 0.312E-01
RMM: 3 -0.136701192855E+01 -0.12907E-02 -0.25580E-04 4930 0.270E-02
RMM: 4 -0.136701224256E+01 -0.31401E-06 -0.14233E-06 3997 0.166E-03
Linear response to external field, progress :
Direction: 1
N E dE d eps ncg rms rms(c)
RMM: 1 -0.898379743375E+00 -0.89838E+00 -0.40123E+00 7390 0.445E+00
RMM: 2 -0.113859777677E+01 -0.24022E+00 -0.14686E-02 8180 0.303E-01 0.153E+00
RMM: 3 -0.111950047968E+01 0.19097E-01 -0.49848E-03 64446 0.154E-01 0.947E-01
RMM: 4 -0.112065083988E+01 -0.11504E-02 -0.18184E-03 66610 0.815E-02 0.505E-01
RMM: 5 -0.114392727474E+01 -0.23276E-01 -0.16131E-03 65698 0.843E-02 0.107E-01
RMM: 6 -0.115067321057E+01 -0.67459E-02 -0.68555E-05 70716 0.184E-02 0.204E-02
RMM: 7 -0.115157230815E+01 -0.89910E-03 -0.44659E-06 71329 0.380E-03 0.470E-03
RMM: 8 -0.115177371886E+01 -0.20141E-03 0.27804E-06 71135 0.906E-04 0.209E-03
RMM: 9 -0.115184492497E+01 -0.71206E-04 -0.33001E-06 69336 0.395E-04 0.975E-04
RMM: 10 -0.115187897422E+01 -0.34049E-04 0.18286E-06 65524 0.222E-04 0.131E-04
RMM: 11 -0.115188122699E+01 -0.22528E-05 -0.52017E-11 41594 0.520E-05 0.271E-05
RMM: 12 -0.115188070492E+01 0.52206E-06 0.00000E+00 20597 0.540E-05 0.739E-06
Linear response to external field, progress :
Direction: 2
N E dE d eps ncg rms rms(c)
RMM: 1 -0.898379742949E+00 -0.89838E+00 -0.40123E+00 7390 0.445E+00
RMM: 2 -0.113859854216E+01 -0.24022E+00 -0.14691E-02 8180 0.303E-01 0.153E+00
RMM: 3 -0.111950054465E+01 0.19098E-01 -0.49858E-03 64441 0.154E-01 0.947E-01
RMM: 4 -0.112065079161E+01 -0.11502E-02 -0.18182E-03 66610 0.815E-02 0.505E-01
RMM: 5 -0.114392726009E+01 -0.23276E-01 -0.16131E-03 65694 0.843E-02 0.107E-01
RMM: 6 -0.115067316852E+01 -0.67459E-02 -0.68552E-05 70716 0.184E-02 0.204E-02
RMM: 7 -0.115157228853E+01 -0.89912E-03 -0.44660E-06 71324 0.380E-03 0.470E-03
RMM: 8 -0.115177371379E+01 -0.20143E-03 0.27804E-06 71134 0.906E-04 0.209E-03
RMM: 9 -0.115184490989E+01 -0.71196E-04 -0.33001E-06 69334 0.395E-04 0.975E-04
RMM: 10 -0.115187898478E+01 -0.34075E-04 0.18286E-06 65522 0.222E-04 0.131E-04
RMM: 11 -0.115188120898E+01 -0.22242E-05 -0.51845E-11 41592 0.520E-05 0.271E-05
RMM: 12 -0.115188070499E+01 0.50399E-06 0.00000E+00 20583 0.541E-05 0.739E-06
Linear response to external field, progress :
Direction: 3
N E dE d eps ncg rms rms(c)
RMM: 1 -0.110999745586E+01 -0.11100E+01 -0.49203E+00 4402 0.458E+00
RMM: 2 -0.136572120827E+01 -0.25572E+00 -0.18867E-02 4918 0.312E-01 0.150E+00
RMM: 3 -0.135832038409E+01 0.74008E-02 -0.33689E-03 33506 0.127E-01 0.832E-01
RMM: 4 -0.139207115877E+01 -0.33751E-01 -0.44654E-03 44727 0.141E-01 0.158E-01
RMM: 5 -0.140347598397E+01 -0.11405E-01 -0.18300E-04 47749 0.285E-02 0.298E-02
RMM: 6 -0.140458540831E+01 -0.11094E-02 -0.43195E-06 47786 0.458E-03 0.142E-02
RMM: 7 -0.140499668486E+01 -0.41128E-03 -0.11653E-06 46532 0.190E-03 0.478E-03
RMM: 8 -0.140527002353E+01 -0.27334E-03 -0.24410E-07 45769 0.106E-03 0.190E-03
RMM: 9 -0.140536889002E+01 -0.98866E-04 -0.83625E-08 45500 0.526E-04 0.153E-04
RMM: 10 -0.140537131788E+01 -0.24279E-05 -0.61652E-12 37585 0.434E-05 0.267E-05
RMM: 11 -0.140537072025E+01 0.59763E-06 -0.46552E-13 18094 0.449E-05 0.654E-06
Linear response DOF= 4
Linear response progress:
Degree of freedom: 1/ 4
N E dE d eps ncg rms rms(c)
RMM: 1 -0.407058241248E+00 -0.40650E+00 -0.13677E+01 44069 0.132E+01
RMM: 2 -0.442907174978E+00 -0.35849E-01 -0.14599E-02 82204 0.237E-01 0.276E-01
RMM: 3 -0.438535910156E+00 0.43713E-02 -0.18914E-04 91057 0.268E-02 0.120E-01
RMM: 4 -0.436273198715E+00 0.22627E-02 -0.73205E-05 91418 0.167E-02 0.452E-02
RMM: 5 -0.435721679668E+00 0.55152E-03 -0.25465E-06 94630 0.353E-03 0.279E-02
RMM: 6 -0.435051602449E+00 0.67008E-03 -0.72767E-06 86260 0.566E-03 0.333E-03
RMM: 7 -0.435100751258E+00 -0.49149E-04 -0.75390E-08 92527 0.607E-04 0.710E-04
RMM: 8 -0.435113821931E+00 -0.13071E-04 -0.20841E-09 92051 0.180E-04 0.229E-04
RMM: 9 -0.435120815865E+00 -0.69939E-05 -0.30006E-10 90900 0.584E-05 0.598E-05
RMM: 10 -0.435121487488E+00 -0.67162E-06 -0.31220E-09 90924 0.118E-05 0.302E-05
Linear response progress:
Degree of freedom: 2/ 4
N E dE d eps ncg rms rms(c)
RMM: 1 -0.379959509840E+00 0.55162E-01 -0.13591E+01 27690 0.128E+01
RMM: 2 -0.416066089276E+00 -0.36107E-01 -0.12978E-02 50419 0.219E-01 0.303E-01
RMM: 3 -0.411970606974E+00 0.40955E-02 -0.15929E-04 56031 0.240E-02 0.126E-01
RMM: 4 -0.409757465632E+00 0.22131E-02 -0.36310E-05 56689 0.120E-02 0.406E-02
RMM: 5 -0.408602351314E+00 0.11551E-02 -0.56068E-06 57024 0.595E-03 0.421E-03
RMM: 6 -0.408617651272E+00 -0.15300E-04 0.18563E-06 59633 0.442E-04 0.244E-03
RMM: 7 -0.408635620874E+00 -0.17970E-04 0.18411E-06 58086 0.291E-04 0.641E-04
RMM: 8 -0.408641011875E+00 -0.53910E-05 0.18633E-06 56614 0.118E-04 0.202E-04
RMM: 9 -0.408645261903E+00 -0.42500E-05 0.18641E-06 58077 0.296E-05 0.106E-04
RMM: 10 -0.408649352531E+00 -0.40906E-05 0.18642E-06 53650 0.246E-05 0.187E-05
RMM: 11 -0.408649561465E+00 -0.20893E-06 0.18653E-06 51030 0.575E-06 0.100E-05
Linear response progress:
Degree of freedom: 3/ 4
N E dE d eps ncg rms rms(c)
RMM: 1 -0.373495709093E+00 0.35154E-01 0.35753E-01 84443 0.730E-01
RMM: 2 -0.373443873376E+00 0.51836E-04 -0.16782E-03 89621 0.770E-02 0.158E-01
RMM: 3 -0.374515236643E+00 -0.10714E-02 -0.12627E-04 94002 0.214E-02 0.957E-02
RMM: 4 -0.375145851142E+00 -0.63061E-03 -0.25124E-05 95403 0.107E-02 0.477E-02
RMM: 5 -0.376118427173E+00 -0.97258E-03 -0.37114E-05 90905 0.894E-03 0.187E-02
RMM: 6 -0.376293701908E+00 -0.17527E-03 -0.24644E-06 93920 0.229E-03 0.877E-03
RMM: 7 -0.376330339839E+00 -0.36638E-04 0.27480E-06 87940 0.131E-03 0.178E-03
RMM: 8 -0.376332285273E+00 -0.19454E-05 0.40939E-06 94531 0.213E-04 0.735E-04
RMM: 9 -0.376331979155E+00 0.30612E-06 0.43160E-06 91744 0.122E-04 0.255E-04
Linear response progress:
Degree of freedom: 4/ 4
N E dE d eps ncg rms rms(c)
RMM: 1 -0.358620553830E+00 0.17711E-01 0.38371E-01 75057 0.739E-01
RMM: 2 -0.359972712868E+00 -0.13522E-02 -0.13964E-03 78559 0.693E-02 0.155E-01
RMM: 3 -0.361412587257E+00 -0.14399E-02 -0.98119E-05 81284 0.185E-02 0.816E-02
RMM: 4 -0.363551436153E+00 -0.21388E-02 -0.91913E-05 79144 0.184E-02 0.205E-02
RMM: 5 -0.363681340486E+00 -0.12990E-03 -0.22470E-06 81790 0.318E-03 0.383E-03
RMM: 6 -0.363688005284E+00 -0.66648E-05 -0.85015E-08 84328 0.538E-04 0.168E-03
RMM: 7 -0.363688726341E+00 -0.72106E-06 0.21954E-09 84625 0.194E-04 0.503E-04
Linear response finished
dielectric constant with ionic contribution
Moderators: Global Moderator, Moderator
-
- Newbie
- Posts: 5
- Joined: Fri Nov 19, 2010 2:29 pm
dielectric constant with ionic contribution
Last edited by deak on Tue Jul 17, 2012 8:40 am, edited 1 time in total.
-
- Administrator
- Posts: 2921
- Joined: Tue Aug 03, 2004 8:18 am
- License Nr.: 458
dielectric constant with ionic contribution
you need not set NSW in that case, VASP automatically determines the degrees of freedom necessary to put up the Hessian Matrix of your system.
Last edited by admin on Fri Jul 20, 2012 2:00 pm, edited 1 time in total.