root / ase / test / replay.py @ 4
Historique | Voir | Annoter | Télécharger (934 octet)
| 1 | 1 | tkerber | from math import sqrt |
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| 2 | 1 | tkerber | from ase import Atoms, Atom |
| 3 | 1 | tkerber | from ase.constraints import FixAtoms |
| 4 | 1 | tkerber | from ase.calculators.emt import EMT |
| 5 | 1 | tkerber | from ase.optimize import QuasiNewton |
| 6 | 1 | tkerber | from ase.io import read |
| 7 | 1 | tkerber | from ase.vibrations import Vibrations |
| 8 | 1 | tkerber | |
| 9 | 1 | tkerber | # Distance between Cu atoms on a (100) surface:
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| 10 | 1 | tkerber | d = 3.6 / sqrt(2) |
| 11 | 1 | tkerber | a = Atoms('Cu',
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| 12 | 1 | tkerber | positions=[(0, 0, 0)], |
| 13 | 1 | tkerber | cell=(d, d, 1.0),
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| 14 | 1 | tkerber | pbc=(True, True, False)) |
| 15 | 1 | tkerber | a *= (2, 2, 1) # 2x2 (100) surface-cell |
| 16 | 1 | tkerber | |
| 17 | 1 | tkerber | # Approximate height of Ag atom on Cu(100) surfece:
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| 18 | 1 | tkerber | h0 = 2.0
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| 19 | 1 | tkerber | a += Atom('Ag', (d / 2, d / 2, h0)) |
| 20 | 1 | tkerber | |
| 21 | 1 | tkerber | if 0: |
| 22 | 1 | tkerber | view(a) |
| 23 | 1 | tkerber | |
| 24 | 1 | tkerber | constraint = FixAtoms(range(len(a) - 1)) |
| 25 | 1 | tkerber | a.set_calculator(EMT()) |
| 26 | 1 | tkerber | a.set_constraint(constraint) |
| 27 | 1 | tkerber | dyn1 = QuasiNewton(a, trajectory='AgCu1.traj', logfile='AgCu1.log') |
| 28 | 1 | tkerber | dyn1.run(fmax=0.1)
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| 29 | 1 | tkerber | |
| 30 | 1 | tkerber | a = read('AgCu1.traj')
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| 31 | 1 | tkerber | a.set_calculator(EMT()) |
| 32 | 1 | tkerber | print a.constraints
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| 33 | 1 | tkerber | dyn2 = QuasiNewton(a, trajectory='AgCu2.traj', logfile='AgCu2.log') |
| 34 | 1 | tkerber | dyn2.replay_trajectory('AgCu1.traj')
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| 35 | 1 | tkerber | dyn2.run(fmax=0.01) |