Ni 111 surface relaxation
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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.
- 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:
- eV.
- (111) surface more stable than (100) surface.
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