[Pw_forum] Is the Graphite surface flat ?
Masoud Nahali
masoudnahali at live.com
Tue Jul 6 13:09:28 CEST 2010
Dear pwscf users
answer to the comments:
(many thanks for your kind attention and help but I could not solve the problem)
to G. Scluuzero: I have used the experimental C-C distance but then I have vc-relaxed the bulk cell and found the new positions. After vc-relax I have used
these coordinates to "relax" the atoms in the cell with vacuum. Also the innermost layer is not graphite-like and is rippled.
to D. C. Andera: this pseudopotential reproduces the experimental cell parameter of the bulk correctly and exactly. the predicted cell parameter in z-direction (c) by the other pseudopotentials is not so exact and sometimes, a difference about 1 angstrom compared to experimental value appears.
to G. Mattioli:
london=.true. closes the atoms in the different layers to each other in the relax calculation and did not solve the problem.
Now I am trying to relax a 5-layer sample and see the result. but it has not completed yet. really I do not know the surface of graphite is "ripple" in the nature (experimentally) or not? I appreciate your help.
> On 07/05/2010 08:19 PM, Masoud Nahali wrote:
> > Dear Quantum Espresso users
> >
> > I optimized the graphite bulk and the layers were completely flat. But
> > when I try to "relax" the graphite surface (slab 2*2 with 3 monolayer)
> > with 10 angstrom vacuum all the layers become extremely ripple!!! I
> > can not find the problem. May it related to the number of layers?
> > anyhow the number of layers is like the bulk. Your help would be a
> > great gift.
G. Scluuzero:
> > __
> Are you using the experimental or the theoretical value for the in-plane
> (graphene) C-C distance? I guess that the PBE value is larger than the
> experimental one, so that if you start from the experimental C-C
> distance in the graphene layer and let everything relax, then the atoms
> would like to go towards the theoretical equilibrium distance and this
> may cause the rippled structure.
> Secondly, I don't know if you can pretend that the innermost layer is
> graphite bulk-like, having only three layers in total.
Dal Corso Andrea :
> Check the pseudopotential. This is a PP with a core hole for special
> purposes not for standard simulations.
Giuseppe Mattioli :
> Dear Masoud
> apart from the pseudo problem issued by Andrea, you could try the keyword
> london=.true.
> It adds a Van der Waals contribution to total energy and it is likely to
> improve the interlayer interactions in your system.
> Hope this helps
> Giuseppe
input file:
&CONTROL
calculation = "relax",
pseudo_dir =
"/home/koa/soft/qe4.2/espresso-4.2/pseudo",
outdir =
"/home/koa/tmp",
etot_conv_thr= 1.0D-4,
forc_conv_thr= 1.0D-3,
nstep=150,
/
&SYSTEM
ibrav = 4,
a =
4.9318,
b = 4.9318,
c = 16.7029,
cosab = -0.5,
cosac = 1.0,
cosbc = 1.0,
nat = 24,
ntyp = 1,
ecutwfc = 40.D0,
ecutrho = 400.D0,
occupations = 'smearing'
smearing ='mp',
degauss = 0.01,
nspin = 2,
starting_magnetization(1)= 1.0,
/
&ELECTRONS
conv_thr = 1.D-6,
mixing_beta = 0.7D0,
diagonalization = "david",
/
&IONS
ion_dynamics="bfgs"
/
ATOMIC_SPECIES
C
12.0107 C.star1s-pbe-rrkjus.UPF
ATOMIC_POSITIONS {angstrom}
C
0.000000 0.000000 0.000000
C 2.465900 0.000000
0.000000
C -1.232950 2.135532 0.000000
C 1.232950
2.135532 0.000000
C 0.000000 1.423688 0.000000
C
-1.232950 3.559220 0.000000
C 2.465900 1.423688
0.000000
C 1.232950 3.559220 0.000000
C 0.000000
0.000000 3.351450
C 2.465900 0.000000 3.351450
C
-1.232950 2.135532 3.351450
C 1.232950 2.135532
3.351450
C 1.232950 0.711844 3.351450
C 0.000000
2.847376 3.351450
C 3.698850 0.711844 3.351450
C
2.465900 2.847376 3.351450
C 0.000000 0.000000
6.702900
C 2.465900 0.000000 6.702900
C -1.232950
2.135532 6.702900
C 1.232950 2.135532 6.702900
C
0.000000 1.423688 6.702900
C -1.232950 3.559220
6.702900
C 2.465900 1.423688 6.702900
C 1.232950
3.559220 6.702900
K_POINTS {automatic}
4 4 1 1 1 1
out
put (optimized positions):
C 0.000000000
-0.000000000 -0.686394528
C 2.465900000 -0.003714144
-0.758610095
C -1.229733457 2.137389072 -0.758610095
C
1.229733457 2.137389072 -0.758610095
C 0.000000000
1.427474855 -0.213813075
C -1.229670488 3.557326573
-0.213813075
C 2.465900000 1.423688000 -0.285079086
C
1.229670488 3.557326573 -0.213813075
C -0.000000000
0.000000000 3.630366631
C 2.465900000 -0.014904710
3.544792504
C -1.220042143 2.142984355 3.544792504
C
1.220042143 2.142984355 3.544792504
C 1.220249305
0.704511250 3.106073641
C 0.000000000 2.847376000
3.022325711
C 3.711550695 0.704511250 3.106073641
C
2.465900000 2.862041499 3.106073641
C 0.000000000
0.000000000 7.468882932
C 2.465900000 0.008344370
7.466151214
C -1.240176436 2.131359815 7.466151214
C
1.240176436 2.131359815 7.466151214
C 0.000000000
1.414904155 6.963129179
C -1.240557033 3.563611923
6.963129179
C 2.465900000 1.423688000 6.961528237
C
1.240557033 3.563611923 6.963129179
Many Thanks
Masoud Nahali
Sharif
University of Technology
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