[Pw_forum] Graphene structure
Gabriele Sclauzero
sclauzer at sissa.it
Mon Nov 22 14:00:19 CET 2010
Ti has an open d shell in valence. Why don't you treat the system as metallic (i.e. use smearing)? Moreover you might need to take into account spin-polarization as well (nspin=2).
HTH
GS
Il giorno 22/nov/2010, alle ore 13.47, Ettore Baldini Neto ha scritto:
> Dear QE users,
>
> I'm kinda new with quantum espresso. I'm trying to relax a Graphene structure with 32C atoms plus one Ti atom at a given position and the structure do not converge.
> In what follows I copy the input. Could anyone give-me some hint? Is there anything wrong or that can be improved? I'm using the pp's from the QE data base. I'm planning to generate my own pp's soon.
> I'm using a k-point grid of 6x6x1 since with SIESTA (dzp basis) the energy and force convergence is achieved without problem.
>
> With best regards,
>
> ************************************************************
> Dr. Ettore Baldini-Neto
> Wernher von Braun Center for Advanced Research
> Campinas, Brazil.
> ************************************************************
>
> &CONTROL
> title = 'Graphene mono layer'
> calculation = "relax" ,
> restart_mode = 'from_scratch' ,
> outdir='/home/usuarios/baldini/espresso-4.2.1/tmp/' ,
> pseudo_dir = '/home/usuarios/baldini/espresso-4.2.1/pseudo' ,
> etot_conv_thr = 1.0E-4 ,
> forc_conv_thr = 1.0D-3 ,
> nstep=50,
> dt=40,
> prefix='1MLG_Ti_H2',
> /
> &SYSTEM
> ibrav = 0.,
> ntyp = 2 ,
> nat = 33 ,
> ecutwfc = 50.0 ,
> ecutrho = 400.0,
> /
> &ELECTRONS
> electron_maxstep = 300.,
> conv_thr = 1.0d-8 ,
> mixing_mode = 'plain',
> mixing_beta = 0.5,
> diagonalization = 'cg' ,
> diago_cg_maxiter = 50,
> /
> &IONS
> /
> CELL_PARAMETERS
> 16.12131954 9.383047808 0.0000000
> 0.00000000 18.658162370 0.0000000
> 0.0000000 0.0000000 56.6893424
> ATOMIC_SPECIES
> C 12.0107 C.pbe-van_ak.UPF
> Ti 47.8670 Ti.pbe-sp-van_ak.UPF
> ATOMIC_POSITIONS angstrom
> C 2.89163 7.40219 1.8862
> C 3.59292 8.63832 1.8826
> C 3.60349 6.16702 1.8884
> C 5.0186 8.64501 1.8612
> C 5.0215 6.16598 1.8904
> C 5.73302 7.40522 1.8718
> C 1.47184 7.39616 1.891
> C 2.89112 9.87066 1.886
> C 2.89471 4.93264 1.8916
> C 5.73319 9.8885 1.8612
> C 5.73643 4.9413 1.8924
> C 7.16348 7.41203 1.882
> C 1.47474 4.9269 1.8924
> C 0.762281 8.62783 1.8946
> C 0.763134 6.16172 1.8914
> C 1.4715 9.86335 1.8934
> C 3.60341 11.1095 1.8868
> C 5.02124 11.1239 1.882
> C 3.60512 3.70156 1.8932
> C 5.02645 3.70789 1.891
> C 7.87807 8.65532 1.8816
> C 7.16373 9.89497 1.872
> C 7.16203 4.94814 1.8954
> C 7.87619 6.17677 1.8996
> C 5.73634 12.3522 1.8872
> C 0.772689 3.69102 1.898
> C 0.762793 1.22003 1.8968
> C 7.87645 11.1337 1.8894
> C 7.16203 12.3587 1.889
> C 7.87201 13.5922 1.8942
> C 2.89479 2.46619 1.8922
> C 1.47482 2.45878 1.8952
> Ti 6.41604 8.65974 3.74
> K_POINTS {automatic}
> 6.0 6.0 1.0 1.0 1.0 1.0
>
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§ Gabriele Sclauzero, EPFL SB ITP CSEA
PH H2 462, Station 3, CH-1015 Lausanne
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