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# -*- coding: utf-8 -*- | ||
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import sys | ||
import os | ||
import numpy as np | ||
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# add a reference to load the Sphecerix library | ||
sys.path.append(os.path.join(os.path.dirname(__file__), '..')) | ||
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from sphecerix import Molecule, BasisFunction, SymmetryOperations,\ | ||
visualize_matrices, CharacterTable, ProjectionOperator | ||
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def main(): | ||
mol = Molecule() | ||
mol.add_atom('C', 0.0000000015, -1.3868467444, 0.0000000000, unit='angstrom') | ||
mol.add_atom('C', 1.2010445126, -0.6934233709, 0.0000000000, unit='angstrom') | ||
mol.add_atom('C', 1.2010445111, 0.6934233735, 0.0000000000, unit='angstrom') | ||
mol.add_atom('C', -0.0000000015, 1.3868467444, 0.0000000000, unit='angstrom') | ||
mol.add_atom('C', -1.2010445126, 0.6934233709, 0.0000000000, unit='angstrom') | ||
mol.add_atom('C', -1.2010445111, -0.6934233735, 0.0000000000, unit='angstrom') | ||
mol.add_atom('H', 0.0000000027, -2.4694205285, 0.0000000000, unit='angstrom') | ||
mol.add_atom('H', 2.1385809117, -1.2347102619, 0.0000000000, unit='angstrom') | ||
mol.add_atom('H', 2.1385809090, 1.2347102666, 0.0000000000, unit='angstrom') | ||
mol.add_atom('H', -0.0000000027, 2.4694205285, 0.0000000000, unit='angstrom') | ||
mol.add_atom('H', -2.1385809117, 1.2347102619, 0.0000000000, unit='angstrom') | ||
mol.add_atom('H', -2.1385809090, -1.2347102666, 0.0000000000, unit='angstrom') | ||
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molset = { | ||
'C': [BasisFunction(2,0,0)], | ||
'H': [] | ||
} | ||
mol.build_basis(molset) | ||
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symops = SymmetryOperations(mol) | ||
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# E | ||
symops.add('identity') | ||
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# 2C6 | ||
symops.add('rotation', '6+', np.array([0,0,1]), 2.0 * np.pi / 6) | ||
symops.add('rotation', '6-', np.array([0,0,1]), -2.0 * np.pi / 6) | ||
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# 2C3 | ||
symops.add('rotation', '3+', np.array([0,0,1]), 2.0 * np.pi / 3) | ||
symops.add('rotation', '3-', np.array([0,0,1]), -2.0 * np.pi / 3) | ||
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# C2 | ||
symops.add('rotation', '2', np.array([0,0,1]), np.pi) | ||
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# 3C2' | ||
for i in range(0,3): | ||
symops.add('rotation', '2,%i' % i, np.array([np.sin(i * 2.0 * np.pi / 3), | ||
np.cos(i * 2.0 * np.pi / 3), | ||
0.0]), np.pi) | ||
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# 3C2'' | ||
for i in range(0,3): | ||
symops.add('rotation', '2,%i' % i, np.array([np.sin(i * 2.0 * np.pi * (1./3 + 1./6)), | ||
np.cos(i * 2.0 * np.pi * (1./3 + 1./6)), | ||
0.0]), np.pi) | ||
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# inversion | ||
symops.add('inversion') | ||
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# 2S3 | ||
symops.add('improper', '3+', np.array([0,0,1]), 2.0 * np.pi / 3) | ||
symops.add('improper', '3-', np.array([0,0,1]), -2.0 * np.pi / 3) | ||
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# 2S6 | ||
symops.add('improper', '6+', np.array([0,0,1]), 2.0 * np.pi / 6) | ||
symops.add('improper', '6-', np.array([0,0,1]), -2.0 * np.pi / 6) | ||
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# sigma_h | ||
symops.add('mirror', 'h(xy)', np.array([0,0,1])) | ||
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# sigma_d | ||
for i in range(0,3): | ||
symops.add('mirror', 'd,%i' % i, np.array([np.sin(i * 2.0 * np.pi * (1./3 + 1./6)), | ||
np.cos(i * 2.0 * np.pi * (1./3 + 1./6)), | ||
0.0])) | ||
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# sigma_v | ||
for i in range(0,3): | ||
symops.add('mirror', 'v,%i' % i, np.array([np.cos(i * 2.0 * np.pi / 3), | ||
np.sin(i * 2.0 * np.pi / 3), | ||
0.0])) | ||
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symops.run() | ||
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visualize_matrices(symops.operation_matrices, | ||
[op.name for op in symops.operations], | ||
[bf.name for bf in symops.mol.basis], | ||
xlabelrot=90, figsize=(24,32), numcols=4) | ||
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# print result LOT | ||
ct = CharacterTable('d6h') | ||
print(ct.lot(np.trace(symops.operation_matrices, axis1=1, axis2=2))) | ||
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# apply projection operator | ||
po = ProjectionOperator(ct, symops) | ||
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mos = po.build_mos(verbose=True) | ||
newmats = [mos @ m @ mos.transpose() for m in symops.operation_matrices] | ||
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visualize_matrices(newmats, | ||
[op.name for op in symops.operations], | ||
['$\phi_{%i}$' % (i+1) for i in range(len(symops.mol.basis))], | ||
figsize=(24,32), numcols=4) | ||
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if __name__ == '__main__': | ||
main() |
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{ | ||
"name":"d6h", | ||
"classes": [ | ||
{ | ||
"symbol": "E", | ||
"multiplicity": 1 | ||
}, | ||
{ | ||
"symbol": "C6(z)", | ||
"multiplicity": 2 | ||
}, | ||
{ | ||
"symbol": "C3", | ||
"multiplicity": 2 | ||
}, | ||
{ | ||
"symbol": "C2", | ||
"multiplicity": 1 | ||
}, | ||
{ | ||
"symbol": "C2'", | ||
"multiplicity": 3 | ||
}, | ||
{ | ||
"symbol": "C2''", | ||
"multiplicity": 3 | ||
}, | ||
{ | ||
"symbol": "i", | ||
"multiplicity": 1 | ||
}, | ||
{ | ||
"symbol": "S3", | ||
"multiplicity": 2 | ||
}, | ||
{ | ||
"symbol": "S6", | ||
"multiplicity": 2 | ||
}, | ||
{ | ||
"symbol": "sigma(h)", | ||
"multiplicity": 1 | ||
}, | ||
{ | ||
"symbol": "sigma(d)", | ||
"multiplicity": 3 | ||
}, | ||
{ | ||
"symbol": "sigma(v)", | ||
"multiplicity": 3 | ||
} | ||
], | ||
"symmetry_groups": [ | ||
{ | ||
"symbol": "A1g", | ||
"characters": [1,1,1,1,1,1,1,1,1,1,1,1] | ||
}, | ||
{ | ||
"symbol": "A2g", | ||
"characters": [1,1,1,1,-1,-1,1,1,1,1,-1,-1] | ||
}, | ||
{ | ||
"symbol": "B1g", | ||
"characters": [1,-1,1,-1,1,-1,1,-1,1,-1,1,-1] | ||
}, | ||
{ | ||
"symbol": "B2g", | ||
"characters": [1,-1,1,-1,-1,1,1,-1,1,-1,-1,1] | ||
}, | ||
{ | ||
"symbol": "E1g", | ||
"characters": [2,1,-1,-2,0,0,2,1,-1,-2,0,0] | ||
}, | ||
{ | ||
"symbol": "E2g", | ||
"characters": [2,-1,-1,2,0,0,2,-1,-1,2,0,0] | ||
}, | ||
{ | ||
"symbol": "A1u", | ||
"characters": [1,1,1,1,1,1,-1,-1,-1,-1,-1,-1] | ||
}, | ||
{ | ||
"symbol": "A2u", | ||
"characters": [1,1,1,1,-1,-1,-1,-1,-1,-1,1,1] | ||
}, | ||
{ | ||
"symbol": "B1u", | ||
"characters": [1,-1,1,-1,1,-1,-1,1,-1,1,-1,1] | ||
}, | ||
{ | ||
"symbol": "B2u", | ||
"characters": [1,-1,1,-1,-1,1,-1,1,-1,1,1,-1] | ||
}, | ||
{ | ||
"symbol": "E1u", | ||
"characters": [2,1,-1,-2,0,0,-2,-1,1,2,0,0] | ||
}, | ||
{ | ||
"symbol": "E2u", | ||
"characters": [2,-1,-1,2,0,0,-2,1,1,-2,0,0] | ||
} | ||
] | ||
} |