[CPMD-list] Ag PP

Ari P Seitsonen Ari.P.Seitsonen at iki.fi
Thu May 27 10:11:14 CEST 2004


Dear Alexander,

  The d as local component for the Ag pseudo doesn't look very good (my
next concern would be for how suitable BLYP is for such a system with
transition metals).

    Greetings,

       apsi

-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-
 Ari Paavo Seitsonen / Ari.P.Seitsonen at iki.fi / http://www.iki.fi/~apsi/
 Tel +41 1 635 44 97 / Fax +41 1 635 68 38 / GSM +41 79 719 09 35      
 Anschrift: Physikalisch Chemisches Institut (PCI), Universität Zürich (UniZh)
 Indirizzo: Winterthurerstraße 190, CH-8057 Zürich
 Address:   Schweiz / Svizzera / Suisse / Svizra / Switzerland

On Thu, 27 May 2004, Alexander Martins Silva wrote:

>        Hi,
> 
>        My imput is the following:
> 
> &CPMD
> 
>   OPTIMIZE WAVEFUNCTION
> 
>   MAXSTEP
> 
>   1000
> 
>   STRUCTURE BONDS ANGLES
> 
> &END
> 
> &DFT
> 
>   NEWCODE
> 
>   FUNCTIONAL BLYP
> 
> &END
> 
> &SYSTEM
> 
>   ANGSTROM
> 
>   SYMMETRY
> 
>   1
> 
>   CELL
> 
>   8.2554  1.0000 1.0000  0  0  0
> 
>   CUTOFF
> 
>   70.0
> 
> &END
> 
> &ATOMS
> 
> *AG_MT_BLYP_1.8     KLEINMAN-BYLANDER
> 
>   LMAX=D
> 
>   3
> 
>     .....
> 
> *H_MT_BLYP
> 
>   LMAX=S
> 
>   1
> 
>     ......
> 
> &END
> 
> 
>        I don't know much about some keywords like LMAX: what are the 
> criteria used? I'm trying to carry out another calculation and I'm 
> seeing the same problems... I dont' know why...  where are the mistakes?
> 
>        Alexander.
> 
> 
> Ari P Seitsonen wrote:
> 
> >Dear Alexander,
> >
> >  How many silver atoms do you now have in your system? Like Axel wrote it 
> >might be that there are so many states close to the Fermi energy - ehmm, 
> >better said that there might be many occupied and unoccupied states 
> >closeby, and during the optimisation they change the ordering. If you are 
> >sure that there is a gap (e.g. you have calculated the same system with a 
> >cluster code) there might be some parameters which could help, otherwise 
> >you might want to switch to fractional occupation numbers (FREE ENERGY 
> >FUNCTIONAL) and a broadening of the occupation numbers.
> >
> >  Just a thought...
> >
> >    Greetings from Karelia/Finland and Zurich,
> >
> >       apsi
> >
> >PS Just a detail, do you use the s or p as the local component of the 
> >  pseudo? And how high is the total energy at the first step?
> >
> >-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-=*=-
> > Ari Paavo Seitsonen / Ari.P.Seitsonen at iki.fi / http://www.iki.fi/~apsi/
> > Tel +41 1 635 44 97 / Fax +41 1 635 68 38 / GSM +41 79 719 09 35      
> > Anschrift: Physikalisch Chemisches Institut (PCI), Universität Zürich (UniZh)
> > Indirizzo: Winterthurerstraße 190, CH-8057 Zürich
> > Address:   Schweiz / Svizzera / Suisse / Svizra / Switzerland
> >
> >On Sat, 22 May 2004, Alexander Martins Silva wrote:
> >
> >  
> >
> >>       Hi,
> >>
> >>          I'm using a blyp PP from a colleague of this list ( ...Please, 
> >>forgive me, I have deleted your email accidentally... Did you have these 
> >>same problems? ...), and I've realized a little improvement, but there 
> >>is oscilations and the excessive number of iteractions in the 
> >>wavefunction optimization yet. As suggested for you, I change the 
> >>minimizer from ODIIS to PCG, and with this approach the oscillations 
> >>have finished, but the convergence stils slow:
> >>...
> >>
> >> 407  1.293E-03   5.452E-05    -131.750308   -2.013E-05     54.93
> >>
> >> LINE SEARCH : LAMBDA=.176           ENERGY =          -131.75035
> >>
> >> 408  1.302E-03   5.516E-05    -131.750328   -2.013E-05     55.04
> >>
> >> LINE SEARCH : LAMBDA=.165           ENERGY =          -131.75037
> >>
> >> 409  1.150E-03   5.651E-05    -131.750350   -2.155E-05     54.81
> >>
> >> LINE SEARCH : LAMBDA=.171           ENERGY =          -131.75039
> >>
> >> 410  1.486E-03   5.603E-05    -131.750371   -2.137E-05     54.76
> >>
> >> LINE SEARCH : LAMBDA=.172           ENERGY =          -131.75041
> >>...
> >>
> >>
> >>       What others parameters should I change to resolve this problem?  
> >>Another question: Is there another code for TM pseudopotentials besides 
> >>the Gianozzi's one? 
> >>
> >>      Alexander.
> >>
> >>       Thanks,
> >>
> >>          Alexander.
> >>
> >>
> >>Axel Kohlmeyer wrote:
> >>
> >>    
> >>
> >>>On Fri, 21 May 2004, alex.msilva wrote:
> >>>
> >>>AM> Hi,
> >>>
> >>>hello alexander,
> >>>
> >>>AM> 
> >>>AM>    I´m trying to obtain some results for a 
> >>>AM> little Ag cluster, so I must to generate a PP 
> >>>AM> for this atom, using the Gianozzi´s code. After 
> >>>AM> that, I have done some tests to validate this 
> >>>AM> PP. I found that a simple optimization 
> >>>AM> wavefunction calculation were evaluated after a 
> >>>AM> slow convergence of more than 100 steps. Is this 
> >>>AM> wrong? What can I do to improve this PP?
> >>>
> >>>i have noticed, that systems containing transition
> >>>metal atoms frequently have convergence issues,
> >>>especially for larger systems.
> >>>
> >>>you may want to try PCG MINIMZE instead of the
> >>>default ODIIS minimizer. also sometimes the 
> >>>convergence improves with increasing the cutoff
> >>>a bit.
> >>>
> >>>as for the quality of your pseudopotential,
> >>>there are two Ag pseudos (one with 1 valence electron
> >>>and one with 11 valence electrons) in the 
> >>>goedecker-hartwigsen pseudopotential library for LDA.
> >>>if your pseudo is using LDA, or you recreate it
> >>>for LDA, you could compare your results.
> >>>
> >>>hope this helps,
> >>>	axel.
> >>>
> >>>AM> 
> >>>AM> 
> >>>AM> Alexander.
> >>>AM>  
> >>>AM> __________________________________________________________________________
> >>>AM> Acabe com aquelas janelinhas que pulam na sua tela.
> >>>AM> AntiPop-up UOL - É grátis!
> >>>AM> http://antipopup.uol.com.br/
> >>>AM> 
> >>>AM> 
> >>>AM> _______________________________________________
> >>>AM> CPMD-list mailing list
> >>>AM> CPMD-list at cpmd.org
> >>>AM> http://www.cpmd.org/mailman/listinfo/cpmd-list
> >>>AM> 
> >>>AM> 
> >>>
> >>> 
> >>>
> >>>      
> >>>
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> >>
> >>    
> >>
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> >  
> >
> 
> 



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