예제 #1
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# Ground-state calculation
from gpaw import GPAW
calc = GPAW(mode='lcao',
            h=0.3,
            basis='dzp',
            setups={'Na': '1'},
            poissonsolver=poissonsolver,
            convergence={'density': 1e-8})
atoms.set_calculator(calc)
energy = atoms.get_potential_energy()
calc.write('gs.gpw', mode='all')

# Time-propagation calculation
from gpaw.lcaotddft import LCAOTDDFT
from gpaw.lcaotddft.dipolemomentwriter import DipoleMomentWriter
# Read converged ground-state file
td_calc = LCAOTDDFT('gs.gpw')
# Attach any data recording or analysis tools
DipoleMomentWriter(td_calc, 'dm.dat')
# Kick
td_calc.absorption_kick([0.0, 0.0, 1e-5])
# Propagate
td_calc.propagate(10, 3000)
# Save the state for restarting later
td_calc.write('td.gpw', mode='all')

# Analyze the results
from gpaw.tddft.spectrum import photoabsorption_spectrum
photoabsorption_spectrum('dm.dat', 'spec.dat')
예제 #2
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파일: td.py 프로젝트: thonmaker/gpaw
from gpaw.lcaotddft import LCAOTDDFT
from gpaw.lcaotddft.dipolemomentwriter import DipoleMomentWriter
from gpaw.lcaotddft.wfwriter import WaveFunctionWriter

# Read the ground-state file
td_calc = LCAOTDDFT('gs.gpw', txt='td.out')

# Attach any data recording or analysis tools
DipoleMomentWriter(td_calc, 'dm.dat')
WaveFunctionWriter(td_calc, 'wf.ulm')

# Kick and propagate
td_calc.absorption_kick([1e-5, 0., 0.])
td_calc.propagate(20, 1500)

# Save the state for restarting later
td_calc.write('td.gpw', mode='all')
예제 #3
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from ase import Atoms
from gpaw.tddft import photoabsorption_spectrum
from gpaw import PoissonSolver
from gpaw.lcaotddft.tddfpt import DensityCollector
from gpaw.lcaotddft import LCAOTDDFT

atoms = Atoms('Na8', positions=[[i * 3.0, 0, 0] for i in range(8)])
atoms.center(vacuum=5.0)

# Calculate all bands
td_calc = LCAOTDDFT(basis='dzp',
                    setups={'Na': '1'},
                    xc='LDA',
                    h=0.3,
                    nbands=4,
                    convergence={'density': 1e-7},
                    poissonsolver=PoissonSolver(eps=1e-14,
                                                remove_moment=1 + 3 + 5))
atoms.set_calculator(td_calc)
atoms.get_potential_energy()
td_calc.write('Na8_gs.gpw', mode='all')

td_calc = LCAOTDDFT('Na8_gs.gpw')
td_calc.attach(DensityCollector('Na8.TdDen', td_calc))
td_calc.absorption_kick([1e-4, 0.0, 0.0])
td_calc.propagate(20, 1000, 'Na8.dm')

photoabsorption_spectrum('Na8.dm', 'Na8.spec', width=0.15)
예제 #4
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            setups=dict(Na='1'),
            basis='sz(dzp)',
            mode='lcao',
            xc='oldLDA',
            poissonsolver=PoissonSolver(eps=1e-16),
            convergence={'density': 1e-8},
            txt='gs.out')
atoms.set_calculator(calc)
energy = atoms.get_potential_energy()
calc.write('gs.gpw', mode='all')

# Time-propagation calculation
td_calc = LCAOTDDFT('gs.gpw', txt='td.out')
DipoleMomentWriter(td_calc, 'dm.dat')
td_calc.absorption_kick([0, 0, 1e-5])
td_calc.propagate(30, 150)
photoabsorption_spectrum('dm.dat',
                         'spec.dat',
                         e_max=10,
                         width=0.5,
                         delta_e=0.1)

# LrTDDFT2 calculation
calc = GPAW('gs.gpw', txt='lr.out')
lr = LrTDDFT2('lr2', calc, fxc='LDA')
lr.calculate()
lr.get_spectrum('lr_spec.dat', 0, 10.1, 0.1, width=0.5)
world.barrier()

# Scale spectra due to slightly different definitions
spec1_ej = np.loadtxt('spec.dat')
예제 #5
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파일: timelimit.py 프로젝트: thonmaker/gpaw
# Atoms
atoms = molecule('Na2')
atoms.center(vacuum=4.0)

# Ground-state calculation that will never converge
maxiter = 100
calc = GPAW(mode='lcao',
            basis='sz(dzp)',
            setups='1',
            convergence={'density': 1e-100},
            maxiter=maxiter)
atoms.set_calculator(calc)

tl = TimeLimiter(calc, timelimit=0, output='scf.txt')
tl.reset('scf', min_updates=3)
try:
    atoms.get_potential_energy()
except KohnShamConvergenceError:
    assert calc.scf.maxiter < maxiter, 'TimeLimiter did not break the SCF loop'
else:
    raise AssertionError('SCF loop ended too early')
calc.write('gs.gpw', mode='all')

# Time-propagation calculation that will never finish
td_calc = LCAOTDDFT('gs.gpw')
tl = TimeLimiter(td_calc, timelimit=0, output='tddft.txt')
tl.reset('tddft', min_updates=3)
td_calc.propagate(10, maxiter - td_calc.niter)
assert td_calc.maxiter < maxiter, 'TimeLimiter did not break the TDDFT loop'
예제 #6
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            h=0.4,
            basis='dzp',
            mode='lcao',
            poissonsolver=PoissonSolver(eps=1e-16),
            convergence={'density': 1e-8},
            xc='GLLBSC',
            txt='gs.out')
atoms.set_calculator(calc)
energy = atoms.get_potential_energy()
calc.write('gs.gpw', mode='all')

# Time-propagation calculation
td_calc = LCAOTDDFT('gs.gpw', txt='td.out')
DipoleMomentWriter(td_calc, 'dm.dat')
td_calc.absorption_kick(np.ones(3) * 1e-5)
td_calc.propagate(20, 3)

# Write a restart point
td_calc.write('td.gpw', mode='all')

# Keep propagating
td_calc.propagate(20, 3)

# Restart from the restart point
td_calc = LCAOTDDFT('td.gpw', txt='td2.out')
DipoleMomentWriter(td_calc, 'dm.dat')
td_calc.propagate(20, 3)
world.barrier()

# Check dipole moment file
data_tj = np.loadtxt('dm.dat')
예제 #7
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            basis='dzp',
            mode='lcao',
            poissonsolver=PoissonSolver(eps=1e-16),
            convergence={'density': 1e-8},
            xc='GLLBSC',
            txt='gs.out')
atoms.set_calculator(calc)
energy = atoms.get_potential_energy()
calc.write('gs.gpw', mode='all')

fxc = 'LDA'
# Time-propagation calculation with fxc
td_calc = LCAOTDDFT('gs.gpw', fxc=fxc, txt='td_fxc.out')
DipoleMomentWriter(td_calc, 'dm_fxc.dat')
td_calc.absorption_kick(np.ones(3) * 1e-5)
td_calc.propagate(20, 4)

# Time-propagation calculation with linearize_to_fxc()
td_calc = LCAOTDDFT('gs.gpw', txt='td_lin.out')
td_calc.linearize_to_xc(fxc)
DipoleMomentWriter(td_calc, 'dm_lin.dat')
td_calc.absorption_kick(np.ones(3) * 1e-5)
td_calc.propagate(20, 4)

# Test the equivalence
world.barrier()
ref = np.loadtxt('dm_fxc.dat').ravel()
data = np.loadtxt('dm_lin.dat').ravel()

tol = 1e-9
equal(data, ref, tol)
예제 #8
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convergence = {'density': 1e-6}

# Increase accuracy of Poisson Solver and apply multipole corrections up to l=2
poissonsolver = PoissonSolver(eps=1e-14, remove_moment=1 + 3)

td_calc = LCAOTDDFT(xc='GLLBSC',
                    basis='GLLBSC.dz',
                    h=0.3,
                    nbands=352,
                    convergence=convergence,
                    poissonsolver=poissonsolver,
                    occupations=FermiDirac(0.1),
                    parallel={
                        'sl_default': (8, 8, 32),
                        'band': 2
                    })

atoms.set_calculator(td_calc)
# Relax the ground state
atoms.get_potential_energy()

# For demonstration purposes, save intermediate ground state result to a file
td_calc.write('ag55.gpw', mode='all')

td_calc = LCAOTDDFT('ag55.gpw', parallel={'sl_default': (8, 8, 32), 'band': 2})

td_calc.absorption_kick([1e-5, 0.0, 0.0])
td_calc.propagate(20, 500, 'ag55.dm')

photoabsorption_spectrum('ag55.dm', 'ag55.spec', width=0.2)
예제 #9
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calc = GPAW(nbands=2, h=0.4, setups=dict(Na='1'),
            basis='dzp', mode='lcao',
            poissonsolver=PoissonSolver(eps=1e-16),
            convergence={'density': 1e-8},
            txt='gs.out')
atoms.set_calculator(calc)
energy = atoms.get_potential_energy()
calc.write('gs.gpw', mode='all')

# Time-propagation calculation
td_calc = LCAOTDDFT('gs.gpw', txt='td.out')
DipoleMomentWriter(td_calc, 'dm.dat')
WaveFunctionWriter(td_calc, 'wf.ulm')
WaveFunctionWriter(td_calc, 'wf_split.ulm', split=True)
td_calc.absorption_kick(np.ones(3) * 1e-5)
td_calc.propagate(20, 3)
td_calc.write('td.gpw', mode='all')
td_calc.propagate(7, 3)

# Restart from the restart point
td_calc = LCAOTDDFT('td.gpw', txt='td2.out')
DipoleMomentWriter(td_calc, 'dm.dat')
WaveFunctionWriter(td_calc, 'wf.ulm')
WaveFunctionWriter(td_calc, 'wf_split.ulm')
td_calc.propagate(20, 3)
td_calc.propagate(20, 3)
td_calc.propagate(10, 3)
photoabsorption_spectrum('dm.dat', 'spec.dat')

world.barrier()
ref_i = np.loadtxt('spec.dat').ravel()
예제 #10
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from gpaw import PoissonSolver

# Sodium dimer
atoms = Atoms('Na2', positions=[[0.0, 0.0, 0.0], [3.0, 0.0, 0.0]])
atoms.center(vacuum=3.5)

from gpaw.lcaotddft import LCAOTDDFT

# Increase accuragy of density for ground state
convergence = {'density': 1e-7}

# Increase accuracy of Poisson Solver and apply multipole corrections up to l=1
poissonsolver = PoissonSolver(eps=1e-14, remove_moment=1 + 3)

td_calc = LCAOTDDFT(setups={'Na': '1'},
                    basis='dzp',
                    xc='LDA',
                    h=0.3,
                    nbands=1,
                    convergence=convergence,
                    poissonsolver=poissonsolver)

atoms.set_calculator(td_calc)
# Relax the ground state
atoms.get_potential_energy()

td_calc.absorption_kick([1e-5, 0.0, 0.0])
td_calc.propagate(20, 250, 'Na2.dm')

photoabsorption_spectrum('Na2.dm', 'Na2.spec', width=0.4)
예제 #11
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파일: fxc_is_xc.py 프로젝트: thonmaker/gpaw
            setups=dict(Na='1'),
            basis='dzp',
            mode='lcao',
            poissonsolver=PoissonSolver(eps=1e-16),
            convergence={'density': 1e-8},
            xc='LDA',
            txt='gs.out')
atoms.set_calculator(calc)
energy = atoms.get_potential_energy()
calc.write('gs.gpw', mode='all')

# Time-propagation calculation without fxc
td_calc = LCAOTDDFT('gs.gpw', txt='td.out')
DipoleMomentWriter(td_calc, 'dm.dat')
td_calc.absorption_kick(np.ones(3) * 1e-5)
td_calc.propagate(20, 4)
world.barrier()

# Check dipole moment file
ref = np.loadtxt('dm.dat').ravel()

# Time-propagation calculation with fxc=xc
td_calc = LCAOTDDFT('gs.gpw', fxc='LDA', txt='td_fxc.out')
DipoleMomentWriter(td_calc, 'dm_fxc.dat')
td_calc.absorption_kick(np.ones(3) * 1e-5)
td_calc.propagate(20, 1)
td_calc.write('td_fxc.gpw', mode='all')

# Restart from the restart point
td_calc = LCAOTDDFT('td_fxc.gpw', txt='td_fxc2.out')
DipoleMomentWriter(td_calc, 'dm_fxc.dat')