Coverage for ase / calculators / acn.py: 93.83%
162 statements
« prev ^ index » next coverage.py v7.13.5, created at 2026-03-30 08:22 +0000
« prev ^ index » next coverage.py v7.13.5, created at 2026-03-30 08:22 +0000
1# fmt: off
3import numpy as np
5import ase.units as units
6from ase.calculators.calculator import Calculator, all_changes
7from ase.data import atomic_masses
8from ase.geometry import find_mic
10# Electrostatic constant
11k_c = units.Hartree * units.Bohr
13# Force field parameters
14q_me = 0.206
15q_c = 0.247
16q_n = -0.453
17sigma_me = 3.775
18sigma_c = 3.650
19sigma_n = 3.200
20epsilon_me = 0.7824 * units.kJ / units.mol
21epsilon_c = 0.544 * units.kJ / units.mol
22epsilon_n = 0.6276 * units.kJ / units.mol
23r_mec = 1.458
24r_cn = 1.157
25r_men = r_mec + r_cn
26m_me = atomic_masses[6] + 3 * atomic_masses[1]
27m_c = atomic_masses[6]
28m_n = atomic_masses[7]
31def combine_lj_lorenz_berthelot(sigma, epsilon):
32 """Combine LJ parameters according to the Lorenz-Berthelot rule"""
33 sigma_c = np.zeros((len(sigma), len(sigma)))
34 epsilon_c = np.zeros_like(sigma_c)
36 for ii in range(len(sigma)):
37 sigma_c[:, ii] = (sigma[ii] + sigma) / 2
38 epsilon_c[:, ii] = (epsilon[ii] * epsilon) ** 0.5
39 return sigma_c, epsilon_c
42class ACN(Calculator):
43 implemented_properties = ['energy', 'forces']
44 nolabel = True
46 def __init__(self, rc=5.0, width=1.0):
47 """Three-site potential for acetonitrile.
49 Atom sequence must be:
50 MeCNMeCN ... MeCN or NCMeNCMe ... NCMe
52 When performing molecular dynamics (MD), forces are redistributed
53 and only Me and N sites propagated based on a scheme for MD of
54 rigid triatomic molecules from Ciccotti et al. Molecular Physics
55 1982 (https://doi.org/10.1080/00268978200100942). Apply constraints
56 using the FixLinearTriatomic to fix the geometry of the acetonitrile
57 molecules.
59 rc: float
60 Cutoff radius for Coulomb interactions.
61 width: float
62 Width for cutoff function for Coulomb interactions.
64 References
65 ----------
67 https://doi.org/10.1080/08927020108024509
68 """
69 self.rc = rc
70 self.width = width
71 self.forces = None
72 Calculator.__init__(self)
73 self.sites_per_mol = 3
74 self.pcpot = None
76 def calculate(self, atoms=None,
77 properties=['energy'],
78 system_changes=all_changes):
79 Calculator.calculate(self, atoms, properties, system_changes)
81 Z = atoms.numbers
82 masses = atoms.get_masses()
83 if Z[0] == 7:
84 n = 0
85 me = 2
86 sigma = np.array([sigma_n, sigma_c, sigma_me])
87 epsilon = np.array([epsilon_n, epsilon_c, epsilon_me])
88 else:
89 n = 2
90 me = 0
91 sigma = np.array([sigma_me, sigma_c, sigma_n])
92 epsilon = np.array([epsilon_me, epsilon_c, epsilon_n])
93 assert (Z[n::3] == 7).all(), 'incorrect atoms sequence'
94 assert (Z[1::3] == 6).all(), 'incorrect atoms sequence'
95 assert (masses[n::3] == m_n).all(), 'incorrect masses'
96 assert (masses[1::3] == m_c).all(), 'incorrect masses'
97 assert (masses[me::3] == m_me).all(), 'incorrect masses'
99 R = self.atoms.positions.reshape((-1, 3, 3))
100 pbc = self.atoms.pbc
101 cd = self.atoms.cell.diagonal()
102 nm = len(R)
104 assert (self.atoms.cell == np.diag(cd)).all(), 'not orthorhombic'
105 assert ((cd >= 2 * self.rc) | ~pbc).all(), 'cutoff too large'
107 charges = self.get_virtual_charges(atoms[:3])
109 # LJ parameters
110 sigma_co, epsilon_co = combine_lj_lorenz_berthelot(sigma, epsilon)
112 energy = 0.0
113 self.forces = np.zeros((3 * nm, 3))
115 for m in range(nm - 1):
116 Dmm = R[m + 1:, 1] - R[m, 1]
117 # MIC PBCs
118 Dmm_min, Dmm_min_len = find_mic(Dmm, atoms.cell, pbc)
119 shift = Dmm_min - Dmm
121 # Smooth cutoff
122 cut, dcut = self.cutoff(Dmm_min_len)
124 for j in range(3):
125 D = R[m + 1:] - R[m, j] + shift[:, np.newaxis]
126 D_len2 = (D**2).sum(axis=2)
127 D_len = D_len2**0.5
128 # Coulomb interactions
129 e = charges[j] * charges / D_len * k_c
130 energy += np.dot(cut, e).sum()
131 F = (e / D_len2 * cut[:, np.newaxis])[:, :, np.newaxis] * D
132 Fmm = -(e.sum(1) * dcut / Dmm_min_len)[:, np.newaxis] * Dmm_min
133 self.forces[(m + 1) * 3:] += F.reshape((-1, 3))
134 self.forces[m * 3 + j] -= F.sum(axis=0).sum(axis=0)
135 self.forces[(m + 1) * 3 + 1::3] += Fmm
136 self.forces[m * 3 + 1] -= Fmm.sum(0)
137 # LJ interactions
138 c6 = (sigma_co[:, j]**2 / D_len2)**3
139 c12 = c6**2
140 e = 4 * epsilon_co[:, j] * (c12 - c6)
141 energy += np.dot(cut, e).sum()
142 F = (24 * epsilon_co[:, j] * (2 * c12 -
143 c6) / D_len2 * cut[:, np.newaxis])[:, :, np.newaxis] * D
144 Fmm = -(e.sum(1) * dcut / Dmm_min_len)[:, np.newaxis] * Dmm_min
145 self.forces[(m + 1) * 3:] += F.reshape((-1, 3))
146 self.forces[m * 3 + j] -= F.sum(axis=0).sum(axis=0)
147 self.forces[(m + 1) * 3 + 1::3] += Fmm
148 self.forces[m * 3 + 1] -= Fmm.sum(0)
150 if self.pcpot:
151 e, f = self.pcpot.calculate(np.tile(charges, nm),
152 self.atoms.positions)
153 energy += e
154 self.forces += f
156 self.results['energy'] = energy
157 self.results['forces'] = self.forces
159 def redistribute_forces(self, forces):
160 return forces
162 def get_molcoms(self, nm):
163 molcoms = np.zeros((nm, 3))
164 for m in range(nm):
165 molcoms[m] = self.atoms[m * 3:(m + 1) * 3].get_center_of_mass()
166 return molcoms
168 def cutoff(self, d):
169 x1 = d > self.rc - self.width
170 x2 = d < self.rc
171 x12 = np.logical_and(x1, x2)
172 y = (d[x12] - self.rc + self.width) / self.width
173 cut = np.zeros(len(d)) # cutoff function
174 cut[x2] = 1.0
175 cut[x12] -= y**2 * (3.0 - 2.0 * y)
176 dtdd = np.zeros(len(d))
177 dtdd[x12] -= 6.0 / self.width * y * (1.0 - y)
178 return cut, dtdd
180 def embed(self, charges):
181 """Embed atoms in point-charges."""
182 self.pcpot = PointChargePotential(charges)
183 return self.pcpot
185 def check_state(self, atoms, tol=1e-15):
186 system_changes = Calculator.check_state(self, atoms, tol)
187 if self.pcpot and self.pcpot.mmpositions is not None:
188 system_changes.append('positions')
189 return system_changes
191 def add_virtual_sites(self, positions):
192 return positions # no virtual sites
194 def get_virtual_charges(self, atoms):
195 charges = np.empty(len(atoms))
196 Z = atoms.numbers
197 if Z[0] == 7:
198 n = 0
199 me = 2
200 else:
201 n = 2
202 me = 0
203 charges[me::3] = q_me
204 charges[1::3] = q_c
205 charges[n::3] = q_n
206 return charges
209class PointChargePotential:
210 def __init__(self, mmcharges):
211 """Point-charge potential for ACN.
213 Only used for testing QMMM.
214 """
215 self.mmcharges = mmcharges
216 self.mmpositions = None
217 self.mmforces = None
219 def set_positions(self, mmpositions):
220 self.mmpositions = mmpositions
222 def calculate(self, qmcharges, qmpositions):
223 energy = 0.0
224 self.mmforces = np.zeros_like(self.mmpositions)
225 qmforces = np.zeros_like(qmpositions)
226 for C, R, F in zip(self.mmcharges, self.mmpositions, self.mmforces):
227 d = qmpositions - R
228 r2 = (d**2).sum(1)
229 e = units.Hartree * units.Bohr * C * r2**-0.5 * qmcharges
230 energy += e.sum()
231 f = (e / r2)[:, np.newaxis] * d
232 qmforces += f
233 F -= f.sum(0)
234 self.mmpositions = None
235 return energy, qmforces
237 def get_forces(self, calc):
238 return self.mmforces