N.B., I assume that you are doing something more than a vacancy -- why
should that be charged?

On Mon, Feb 22, 2016 at 6:36 PM, Laurence Marks <l-ma...@northwestern.edu>
wrote:

> I assume that you have correctly changed the number of electrons in both
> case.in2(c) and case.inm.
>
> Beyond that, please execute and send me the output (or the list)
>
> tail -n 50000 *.scf | grep -e :ADIST -e :DIR -e :MV -e GREED -e :FRMS -e
> :ENE -e :CHARG -e PRATT \
> -e :DIS -e "MIXING SC" -e ":RANK" -e PLANE | \
> grep -v -e "with 1.0" -e scheme -e CONTRIBUTION | \
> tail -44
>
> Without some more information about what is going on it is impossible to
> say anything beyond vague and probably incorrect general statements.
>
>
> On Mon, Feb 22, 2016 at 5:45 PM, Hu, Wenhao <wenhao...@uiowa.edu> wrote:
>
>> Hi, all:
>>
>> I met some convergence issue when I made the charged state calculation.
>> The situation is, when I made a charged state calculation, the SCF can’t
>> achieve convergence. But in all neutral and most charged states, this issue
>> won’t show up but only in certain charged states. For your convenience, the
>> calculation I’m making is an isolated vacancy on diamond surface. I
>> observed that the defect levels tend to be highly unlocalized which makes
>> the related bands very dispersive. In this sense, the magnetic moment
>> exhibits to be highly unstable:
>>
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.53572
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.18060
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.10316
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.11329
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.11916
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =   -0.04368
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.06194
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.22852
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.24276
>> :MMTOT:  SPIN MAGNETIC MOMENT IN CELL     =    0.20449
>>
>> Also, By checking the :DIS label:
>>
>> :DIS  :  CHARGE DISTANCE       ( 0.0591612 for atom   49 spin 1)
>> 0.0126272
>> :DIS  :  CHARGE DISTANCE       ( 0.1016792 for atom   49 spin 1)
>> 0.0145533
>> :DIS  :  CHARGE DISTANCE       ( 0.0768202 for atom   49 spin 1)
>> 0.0186368
>> :DIS  :  CHARGE DISTANCE       ( 0.0771968 for atom   49 spin 1)
>> 0.0136267
>> :DIS  :  CHARGE DISTANCE       ( 0.0825579 for atom   49 spin 1)
>> 0.0120297
>> :DIS  :  CHARGE DISTANCE       ( 0.0805263 for atom   49 spin 1)
>> 0.0113403
>> :DIS  :  CHARGE DISTANCE       ( 0.0750162 for atom   49 spin 1)
>> 0.0110824
>> :DIS  :  CHARGE DISTANCE       ( 0.0710646 for atom   49 spin 1)
>> 0.0105623
>> :DIS  :  CHARGE DISTANCE       ( 0.0486714 for atom   49 spin 1)
>> 0.0087271
>> :DIS  :  CHARGE DISTANCE       ( 0.0630542 for atom   49 spin 1)
>> 0.0120210
>>
>> the atom 49 (surface C on the edge of unit cell) seems to be the issue. I
>> doubted it’s due to the k mesh I’m using is too coarse. Thus, I tried a
>> finer k mesh (increase from 3x3x2 to 5x5x2) but it didn't make a difference
>> still. Before using a finer k mesh, can anyone give a suggestion on this?
>> If any other information about my calculation is needed, please let me know.
>>
>> thanks!
>> Wenhao
>>
>>
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>
>
>
> --
> Professor Laurence Marks
> "Research is to see what everybody else has seen, and to think what nobody
> else has thought", Albert Szent-Gyorgi
> www.numis.northwestern.edu ; Corrosion in 4D:
> MURI4D.numis.northwestern.edu
> Partner of the CFW 100% program for gender equity, www.cfw.org/100-percent
> Co-Editor, Acta Cryst A
>



-- 
Professor Laurence Marks
"Research is to see what everybody else has seen, and to think what nobody
else has thought", Albert Szent-Gyorgi
www.numis.northwestern.edu ; Corrosion in 4D: MURI4D.numis.northwestern.edu
Partner of the CFW 100% program for gender equity, www.cfw.org/100-percent
Co-Editor, Acta Cryst A
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