Ni 111 surface relaxation: Difference between revisions
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| {{Sur_sci}} | {{Sur_sci - Tutorial}} | ||
| == Task == | |||
| Relaxation of the first two layers of a Ni (111) surface. | |||
| == Input == | |||
| === {{TAG|POSCAR}} === | |||
| <pre> | |||
|  fcc (111) surface | |||
|   3.53 | |||
|    .70710678  .0000000  .000000 | |||
|  -0.35355339 0.6123724  .000000 | |||
|    .000000    .000000  5.1961524 | |||
|     5 | |||
| selective dynamics | |||
| direct | |||
|    .00000000   .00000000   .00000000  F  F  F | |||
|    .33333333   .66666667   .11111111  F  F  F | |||
|    .66666667   .33333333   .22222222  F  F  F | |||
|    .00000000   .00000000   .33333333  T  T  T | |||
|    .33333333   .66666667   .44444444  T  T  T | |||
| </pre> | |||
| *Similar setup as for {{TAG|Ni 100 surface relaxation}}. | |||
| *Again 2 of 5 layers relaxed. | |||
| *<math>(1-.444)\cdot 5.196 \cdot 3.53 \approx 10.2</math> <math>\AA</math> of vacuum. | |||
| === {{TAG|INCAR}} === | |||
|   general: |   general: | ||
|     {{TAGBL|ISTART}} = 0 |     {{TAGBL|ISTART}} = 0 | ||
| Line 19: | Line 42: | ||
|     {{TAGBL|IBRION}} = 1 |     {{TAGBL|IBRION}} = 1 | ||
| *{{TAG|KPOINTS}} | *Same {{TAG|INCAR}} file as for {{TAG|Ni 100 surface relaxation}}, but spin polarization neglected. | ||
| === {{TAG|KPOINTS}} === | |||
| <pre> | <pre> | ||
| k-points | k-points | ||
| Line 28: | Line 53: | ||
| </pre> | </pre> | ||
| * | == Calculation == | ||
| *N.B.: The setup for the calculation of the "bulk" energy can be found in the ''Ni111clean_rel/bulk'' subdirectory of the tar file. | |||
| *The sample output for the forces should look like the following: | |||
|   POSITION                                       TOTAL-FORCE (eV/Angst) | |||
|  ----------------------------------------------------------------------------------- | |||
|       0.00000      0.00000      0.00000         0.000000      0.000000      0.178848 | |||
|       0.00000      1.44112      2.03805         0.000000      0.000000     -0.060127 | |||
|       1.24804      0.72056      4.07609         0.000000      0.000000      0.004418 | |||
|       0.00000      0.00000      6.11522         0.000000      0.000000      0.036384 | |||
|       0.00000      1.44112      8.14905         0.000000      0.000000     -0.159523 | |||
|   ----------------------------------------------------------------------------------- | |||
|     total drift:                               -0.000084      0.000107     -0.017457 | |||
| </ | *Forces are already small at the beginning (small relaxations for compact surfaces). | ||
| *For surface energy non-spin-polarized bulk nickel as reference: | |||
| **<math>\sigma^{\mathrm{unrel}} = \frac{1}{2} (-25.731 - 5 \cdot (-5.407)) = 0.65</math> eV. | |||
| **(111) surface more stable than (100) surface. | |||
| == Download == | == Download == | ||
| [ | [[Media:Ni111clean_rel.tgz| Ni111clean_rel.tgz]] | ||
| {{Sur_sci}} | |||
| [[Category:Examples]] | [[Category:Examples]] | ||
Latest revision as of 13:56, 14 November 2019
Overview > Ni 100 surface relaxation > Ni 100 surface DOS > Ni 100 surface bandstructure > Ni 111 surface relaxation > CO on Ni 111 surface > Ni 111 surface high precision >  partial DOS of CO on Ni 111 surface > vibrational frequencies of CO on Ni 111 surface > STM of graphite > STM of graphene > collective jumps of a Pt adatom on fcc-Pt (001): Nudged Elastic Band Calculation  > List of tutorials
Task
Relaxation of the first two layers of a Ni (111) surface.
Input
POSCAR
 fcc (111) surface
  3.53
   .70710678  .0000000  .000000
 -0.35355339 0.6123724  .000000
   .000000    .000000  5.1961524
    5
selective dynamics
direct
   .00000000   .00000000   .00000000  F  F  F
   .33333333   .66666667   .11111111  F  F  F
   .66666667   .33333333   .22222222  F  F  F
   .00000000   .00000000   .33333333  T  T  T
   .33333333   .66666667   .44444444  T  T  T
- Similar setup as for Ni 100 surface relaxation.
- Again 2 of 5 layers relaxed.
- [math]\displaystyle{ (1-.444)\cdot 5.196 \cdot 3.53 \approx 10.2 }[/math] [math]\displaystyle{ \AA }[/math] of vacuum.
INCAR
general: ISTART = 0 ICHARG = 2 SYSTEM = clean (111) surface ENMAX = 270 ISMEAR = 2 ; SIGMA = 0.2 ALGO = Fast EDIFF = 1E-6 dynamic: NSW = 100 POTIM = 0.8 IBRION = 1
- Same INCAR file as for Ni 100 surface relaxation, but spin polarization neglected.
KPOINTS
k-points 0 Monkhorst-Pack 9 9 1 0 0 0
Calculation
- N.B.: The setup for the calculation of the "bulk" energy can be found in the Ni111clean_rel/bulk subdirectory of the tar file.
- The sample output for the forces should look like the following:
POSITION                                       TOTAL-FORCE (eV/Angst)
-----------------------------------------------------------------------------------
     0.00000      0.00000      0.00000         0.000000      0.000000      0.178848
     0.00000      1.44112      2.03805         0.000000      0.000000     -0.060127
     1.24804      0.72056      4.07609         0.000000      0.000000      0.004418
     0.00000      0.00000      6.11522         0.000000      0.000000      0.036384
     0.00000      1.44112      8.14905         0.000000      0.000000     -0.159523
-----------------------------------------------------------------------------------
   total drift:                               -0.000084      0.000107     -0.017457
- Forces are already small at the beginning (small relaxations for compact surfaces).
- For surface energy non-spin-polarized bulk nickel as reference:
- [math]\displaystyle{ \sigma^{\mathrm{unrel}} = \frac{1}{2} (-25.731 - 5 \cdot (-5.407)) = 0.65 }[/math] eV.
- (111) surface more stable than (100) surface.
 
Download
Overview > Ni 100 surface relaxation > Ni 100 surface DOS > Ni 100 surface bandstructure > Ni 111 surface relaxation > CO on Ni 111 surface > Ni 111 surface high precision >  partial DOS of CO on Ni 111 surface > vibrational frequencies of CO on Ni 111 surface > STM of graphite > STM of graphene > collective jumps of a Pt adatom on fcc-Pt (001): Nudged Elastic Band Calculation  > List of tutorials
