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include sphecerix/charactertables/*.json |
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figures/* |
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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), | ||
# BasisFunction(2,1,1), # x | ||
# BasisFunction(2,1,-1), # y | ||
BasisFunction(2,1,0)], # z | ||
'H': [BasisFunction(1,0,0)] | ||
} | ||
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(2.0 * np.pi * i/6.), | ||
-np.cos(2.0 * np.pi * i/6.), | ||
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(2.0 * np.pi * (i/6. + 1./12)), | ||
-np.cos(2.0 * np.pi * (i/6. + 1./12)), | ||
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.cos(2.0 * np.pi * (i/6. + 1./12)), | ||
np.sin(2.0 * np.pi * (i/6. + 1./12)), | ||
0.0])) | ||
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# sigma_v | ||
for i in range(0,3): | ||
symops.add('mirror', 'v,%i' % i, np.array([np.cos(2.0 * np.pi * i/6), | ||
np.sin(2.0 * np.pi * i/6), | ||
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, | ||
highlight_groups=po.get_blocks()) | ||
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if __name__ == '__main__': | ||
main() |
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# -*- coding: utf-8 -*- | ||
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import sys | ||
import os | ||
import numpy as np | ||
import matplotlib.pyplot as plt | ||
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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, \ | ||
plot_matrix | ||
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def main(): | ||
mol = Molecule() | ||
mol.add_atom('C', 0.0, 0.0, 0.0, unit='angstrom') | ||
mol.add_atom('Cl', 1,1,1, unit='angstrom') | ||
mol.add_atom('Cl', 1,-1,-1, unit='angstrom') | ||
mol.add_atom('Cl', -1,1,-1, unit='angstrom') | ||
mol.add_atom('Cl', -1,-1,1, unit='angstrom') | ||
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molset = { | ||
'C': [BasisFunction(1,0,0), | ||
BasisFunction(2,0,0), | ||
BasisFunction(2,1,1), | ||
BasisFunction(2,1,-1), | ||
BasisFunction(2,1,0)], | ||
'Cl': [BasisFunction(1,0,0), | ||
BasisFunction(2,1,1), | ||
BasisFunction(2,1,-1), | ||
BasisFunction(2,1,0)] | ||
} | ||
mol.build_basis(molset) | ||
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symops = SymmetryOperations(mol) | ||
symops.add('identity') | ||
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# add C3 rotations | ||
for i in range(0,4): | ||
axis = mol.atoms[i+1][1] | ||
axis /= np.linalg.norm(axis) # normalize axis | ||
for j in range(0,2): | ||
symops.add('rotation', '3,%i' % (i*2+j+1), axis, (-1)**j * 2.0 * np.pi / 3) | ||
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# C2 rotations | ||
for i in range(0,3): | ||
axis = np.zeros(3) | ||
axis[i] = 1.0 | ||
symops.add('rotation', '2,%i' % (i+1), axis, np.pi) | ||
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# S4 rotations | ||
for i in range(0,3): | ||
axis = np.zeros(3) | ||
axis[i] = 1.0 | ||
for j in range(0,2): | ||
symops.add('improper', '4,%i' % (i+1), axis, (-1)**j * np.pi/2) | ||
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# sigma_d mirror planes | ||
ctr = 0 | ||
for i in range(0,4): | ||
axis1 = mol.atoms[i+1][1] | ||
for j in range(i+1,4): | ||
axis2 = mol.atoms[j+1][1] | ||
normal = np.cross(axis1, axis2) | ||
normal /= np.linalg.norm(normal) | ||
ctr += 1 | ||
symops.add('mirror', ',d(%i)' % (ctr), normal) | ||
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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=(36,24), numcols=6) | ||
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# print result LOT | ||
ct = CharacterTable('td') | ||
print(ct.lot(np.trace(symops.operation_matrices, axis1=1, axis2=2))) | ||
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# # apply projection operator | ||
po = ProjectionOperator(ct, symops) | ||
mos = po.build_mos(verbose=True) | ||
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fig, ax = plt.subplots(1,1,dpi=144,figsize=(20,20)) | ||
plot_matrix(ax, mos,[bf.name for bf in symops.mol.basis],None,0) | ||
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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))], | ||
xlabelrot=90, figsize=(36,24), numcols=6, | ||
highlight_groups=po.get_blocks()) | ||
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if __name__ == '__main__': | ||
main() |
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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', 0.0, 0.0, 0.0, unit='angstrom') | ||
mol.add_atom('H', 1,1,1, unit='angstrom') | ||
mol.add_atom('H', 1,-1,-1, unit='angstrom') | ||
mol.add_atom('H', -1,1,-1, unit='angstrom') | ||
mol.add_atom('H', -1,-1,1, unit='angstrom') | ||
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molset = { | ||
'C': [BasisFunction(1,0,0), | ||
BasisFunction(2,0,0), | ||
BasisFunction(2,1,1), | ||
BasisFunction(2,1,-1), | ||
BasisFunction(2,1,0)], | ||
'H': [BasisFunction(1,0,0)] | ||
} | ||
mol.build_basis(molset) | ||
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symops = SymmetryOperations(mol) | ||
symops.add('identity') | ||
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# add C3 rotations | ||
for i in range(0,4): | ||
axis = mol.atoms[i+1][1] | ||
axis /= np.linalg.norm(axis) # normalize axis | ||
for j in range(0,2): | ||
symops.add('rotation', '3,%i' % (i*2+j+1), axis, (-1)**j * 2.0 * np.pi / 3) | ||
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# C2 rotations | ||
for i in range(0,3): | ||
axis = np.zeros(3) | ||
axis[i] = 1.0 | ||
symops.add('rotation', '2,%i' % (i+1), axis, np.pi) | ||
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# S4 rotations | ||
for i in range(0,3): | ||
axis = np.zeros(3) | ||
axis[i] = 1.0 | ||
for j in range(0,2): | ||
symops.add('improper', '4,%i' % (i+1), axis, (-1)**j * np.pi/2) | ||
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# sigma_d mirror planes | ||
ctr = 0 | ||
for i in range(0,4): | ||
axis1 = mol.atoms[i+1][1] | ||
for j in range(i+1,4): | ||
axis2 = mol.atoms[j+1][1] | ||
normal = np.cross(axis1, axis2) | ||
normal /= np.linalg.norm(normal) | ||
ctr += 1 | ||
symops.add('mirror', ',d(%i)' % (ctr), normal) | ||
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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=(18,12), numcols=6) | ||
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# print result LOT | ||
ct = CharacterTable('td') | ||
print(ct.lot(np.trace(symops.operation_matrices, axis1=1, axis2=2))) | ||
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# # apply projection operator | ||
po = ProjectionOperator(ct, symops) | ||
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))], | ||
xlabelrot=90, figsize=(18,12), numcols=6, | ||
highlight_groups=po.get_blocks()) | ||
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if __name__ == '__main__': | ||
main() |
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