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from ase.vibrations.resonant_raman import ResonantRaman
from gpaw.cluster import Cluster
from gpaw import GPAW, FermiDirac
from gpaw.lrtddft import LrTDDFT
h = 0.25
atoms = Cluster('relaxed.traj')
atoms.minimal_box(3.5, h=h)
# relax the molecule
calc = GPAW(h=h, occupations=FermiDirac(width=0.1),
eigensolver='cg', symmetry={'point_group': False},
nbands=10, convergence={'eigenstates':1.e-5,
'bands':4})
atoms.calc = calc
# use only the 4 converged states for linear response calculation
rr = ResonantRaman(atoms, LrTDDFT, exkwargs={'jend':3})
rr.run()
from ase.build import molecule
from ase import optimize
from ase.vibrations.infrared import InfraRed
from gpaw.cluster import Cluster
from gpaw import GPAW, FermiDirac
h = 0.22
atoms = Cluster(molecule('H2'))
atoms.minimal_box(3.5, h=h)
# relax the molecule
calc = GPAW(h=h, occupations=FermiDirac(width=0.1))
atoms.calc = calc
dyn = optimize.FIRE(atoms)
dyn.run(fmax=0.05)
atoms.write('relaxed.traj')
# finite displacement for vibrations
ir = InfraRed(atoms)
ir.run()
from gpaw import GPAW, FermiDirac
from ase.io import read
atoms = read('opt.traj')
calc = GPAW(mode='lcao', basis='sz(dzp)', txt='gpaw.txt',
occupations=FermiDirac(0.1),
setups={'Ag': '11'})
atoms.calc = calc
atoms.center(vacuum=4.0)
atoms.get_potential_energy()
atoms.calc.write('groundstate.gpw')