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add the gamma-point hessian with phonopy #860
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| Original file line number | Diff line number | Diff line change |
|---|---|---|
| @@ -0,0 +1,62 @@ | ||
| #!/usr/bin/env python | ||
| # Copyright 2026 The PySCF Developers. All Rights Reserved. | ||
| # | ||
| # Licensed under the Apache License, Version 2.0 (the "License"); | ||
| # you may not use this file except in compliance with the License. | ||
| # You may obtain a copy of the License at | ||
| # | ||
| # http://www.apache.org/licenses/LICENSE-2.0 | ||
| # | ||
| # Unless required by applicable law or agreed to in writing, software | ||
| # distributed under the License is distributed on an "AS IS" BASIS, | ||
| # WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. | ||
| # See the License for the specific language governing permissions and | ||
| # limitations under the License. | ||
|
|
||
| import numpy as np | ||
| from pyscf import lib | ||
| from pyscf.pbc import gto | ||
|
|
||
| from gpu4pyscf.pbc import dft | ||
| from gpu4pyscf.pbc.hessian import GammaHessian | ||
|
|
||
|
|
||
| a = 5.431 | ||
| cell = gto.Cell() | ||
| cell.a = np.array( | ||
| [ | ||
| [0.0, a / 2, a / 2], | ||
| [a / 2, 0.0, a / 2], | ||
| [a / 2, a / 2, 0.0], | ||
| ] | ||
| ) | ||
| cell.atom = [ | ||
| ["Si", [0.0, 0.0, 0.0]], | ||
| ["Si", [a / 4, a / 4, a / 4]], | ||
| ] | ||
| cell.unit = "Angstrom" | ||
| cell.basis = "gth-dzv" | ||
| cell.pseudo = "gth-pbe" | ||
| cell.precision = 1e-8 | ||
| cell.verbose = 4 | ||
| cell.build() | ||
|
|
||
| mf = dft.RKS(cell, xc="pbe") | ||
| mf.conv_tol = 1e-9 | ||
| mf.kernel() | ||
|
|
||
| hessian = GammaHessian(mf, primitive_matrix=np.eye(3)) | ||
| fc = hessian.kernel() | ||
| frequencies, eigenvectors, dyn_mat = hessian.phonon_modes() | ||
| frequencies_phonopy, _, _ = hessian.phonopy_modes() | ||
|
|
||
| lib.logger.note(mf, "Gamma-point frequencies (cm^-1):") | ||
| for mode, (frequency, frequency_phonopy) in enumerate( | ||
| zip(frequencies, frequencies_phonopy), 1): | ||
| lib.logger.note( | ||
| mf, | ||
| " mode %2d: manual %12.4f phonopy %12.4f", | ||
| mode, | ||
| frequency, | ||
| frequency_phonopy, | ||
| ) |
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|---|---|---|
| @@ -0,0 +1,21 @@ | ||
| # Copyright 2026 The PySCF Developers. All Rights Reserved. | ||
| # | ||
| # Licensed under the Apache License, Version 2.0 (the "License"); | ||
| # you may not use this file except in compliance with the License. | ||
| # You may obtain a copy of the License at | ||
| # | ||
| # http://www.apache.org/licenses/LICENSE-2.0 | ||
| # | ||
| # Unless required by applicable law or agreed to in writing, software | ||
| # distributed under the License is distributed on an "AS IS" BASIS, | ||
| # WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. | ||
| # See the License for the specific language governing permissions and | ||
| # limitations under the License. | ||
|
|
||
| from gpu4pyscf.pbc.hessian.gamma_hessian import ( | ||
| GammaHessian, | ||
| HAS_PHONOPY, | ||
| ) | ||
|
|
||
| __all__ = ["HAS_PHONOPY", "GammaHessian"] | ||
|
|
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| Original file line number | Diff line number | Diff line change |
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| @@ -0,0 +1,275 @@ | ||
| # Copyright 2026 The PySCF Developers. All Rights Reserved. | ||
| # | ||
| # Licensed under the Apache License, Version 2.0 (the "License"); | ||
| # you may not use this file except in compliance with the License. | ||
| # You may obtain a copy of the License at | ||
| # | ||
| # http://www.apache.org/licenses/LICENSE-2.0 | ||
| # | ||
| # Unless required by applicable law or agreed to in writing, software | ||
| # distributed under the License is distributed on an "AS IS" BASIS, | ||
| # WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. | ||
| # See the License for the specific language governing permissions and | ||
| # limitations under the License. | ||
|
|
||
| """ | ||
| EXPERIMENTAL FEATURE | ||
| Numerical Gamma-point force constants and phonon modes. | ||
|
|
||
| Only the analytic (TO) contribution is included. Non-analytic corrections | ||
| (NAC) are not supported. | ||
| """ | ||
|
|
||
| __all__ = [ | ||
| "HAS_PHONOPY", | ||
| "GammaHessian", | ||
| ] | ||
|
|
||
| import copy | ||
| import numpy as np | ||
| from pyscf import lib | ||
| from pyscf.data.nist import BOHR as BOHR_TO_ANGSTROM | ||
| from pyscf.data.nist import HARTREE2EV, AMU2AU, HARTREE2WAVENUMBER, HARTREE2J, PLANCK | ||
| try: | ||
| from phonopy import Phonopy | ||
| from phonopy.structure.atoms import PhonopyAtoms | ||
| HAS_PHONOPY = True | ||
| except ImportError: | ||
| HAS_PHONOPY = False | ||
| from gpu4pyscf.lib import logger | ||
|
|
||
| GRAD_TO_FORCE = -(HARTREE2EV / BOHR_TO_ANGSTROM) | ||
| EV_A2_TO_HA_BOHR2 = BOHR_TO_ANGSTROM**2 / HARTREE2EV | ||
| HARTREE_TO_THZ = HARTREE2J / (PLANCK * 1e12) | ||
|
|
||
|
|
||
| # TODO: in the future, the interfaces should be the same with mol. | ||
| class GammaHessian(lib.StreamObject): | ||
| """Numerical Gamma-point TO Hessian without NAC, seriously q=0, NOT q->0. | ||
|
|
||
| ``primitive_matrix`` maps the input cell to the primitive cell and must | ||
| be supplied explicitly. ``kernel`` stores the corresponding phonopy | ||
| object in ``phonon``. | ||
| """ | ||
|
|
||
| def __init__( | ||
| self, | ||
| mf, | ||
| primitive_matrix, # transformation matrix to primitive cell from unit cell | ||
| displacement=0.01, # angstroms | ||
| force_central_diff=False, | ||
| symmetrize=True, | ||
| ): | ||
| primitive_matrix = np.asarray(primitive_matrix, dtype=np.float64) | ||
| if primitive_matrix.shape != (3, 3): | ||
| raise ValueError("primitive_matrix must have shape (3, 3)") | ||
|
|
||
| self.mf = mf | ||
| self.primitive_matrix = primitive_matrix.copy() | ||
| self.displacement = displacement | ||
| self.force_central_diff = force_central_diff | ||
| self.symmetrize = symmetrize | ||
|
|
||
| self.phonon = None | ||
| self.force_sets = None | ||
| self.force_constants = None | ||
|
|
||
| def kernel(self): | ||
| """Compute the primitive-cell Gamma Hessian in Hartree/Bohr**2. | ||
|
|
||
| The returned shape is ``(3N, 3N)``, where N is the number of atoms | ||
| in the primitive cell defined by ``primitive_matrix``. | ||
| """ | ||
| # TODO: if there is no phonopy, should change the routine to use manual central difference | ||
| if not HAS_PHONOPY: | ||
| raise ImportError( | ||
| "phonopy is required for GammaHessian; install it with " | ||
| "`pip install phonopy`." | ||
| ) | ||
| if not np.isfinite(self.displacement) or self.displacement <= 0: | ||
| raise ValueError("displacement must be a positive finite number") | ||
|
|
||
| self.force_sets = None | ||
| self.force_constants = None | ||
| mf = self.mf | ||
| cell = mf.cell | ||
| natm = cell.natm | ||
| original_coords = cell.atom_coords().copy() # Bohr | ||
| original_atom = copy.deepcopy(cell.atom) | ||
| original_lattice = copy.deepcopy(cell.a) # Bohr | ||
| original_unit = cell.unit | ||
|
|
||
| # default calculator is vasp, default unit in phonopy for vasp: | ||
| # | Distance Atomic mass Force Force constants | ||
| # ----------------------------------------------------------------- | ||
| # VASP | Angstrom AMU eV/Angstrom eV/Angstrom^2 | ||
| unitcell = PhonopyAtoms( | ||
| symbols=[cell.atom_symbol(i) for i in range(natm)], | ||
| cell=np.asarray(cell.lattice_vectors()) * BOHR_TO_ANGSTROM, | ||
| positions=original_coords * BOHR_TO_ANGSTROM, | ||
| masses=np.asarray(cell.atom_mass_list()), | ||
| ) | ||
| self.phonon = Phonopy( | ||
| unitcell, | ||
| supercell_matrix=np.eye(3, dtype=int), | ||
| primitive_matrix=self.primitive_matrix, | ||
| log_level=0, | ||
| ) | ||
| is_plusminus = True if bool(self.force_central_diff) else "auto" | ||
| self.phonon.generate_displacements( | ||
| distance=self.displacement, | ||
| is_plusminus=is_plusminus, | ||
| ) | ||
| displaced_cells = [ | ||
| displaced | ||
| for displaced in self.phonon.supercells_with_displacements | ||
| if displaced is not None | ||
| ] | ||
| logger.info( | ||
| mf, | ||
| "Gamma-point finite-difference Hessian: %d displaced structures, " | ||
| "distance = %.6g Angstrom", | ||
| len(displaced_cells), | ||
| self.displacement, | ||
| ) | ||
|
|
||
| force_sets = [] | ||
| dm0 = mf.make_rdm1() | ||
| try: | ||
| for index, displaced in enumerate(displaced_cells, 1): | ||
| cell.set_geom_(displaced.positions, unit="Angstrom") | ||
|
Collaborator
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. cell = cell.set_geom_(displaced.positions, unit="Angstrom", inplace=False) |
||
| mf_disp = mf.copy().reset(cell) | ||
| logger.info( | ||
| mf, | ||
| "Running displaced SCF and gradient %d/%d", | ||
| index, | ||
| len(displaced_cells), | ||
| ) | ||
| mf_disp.kernel(dm0=dm0) | ||
| if not mf_disp.converged: | ||
| logger.warn( | ||
| mf, | ||
| "SCF did not converge for displaced structure %d/%d", | ||
| index, | ||
| len(displaced_cells), | ||
| ) | ||
| raise RuntimeError("SCF did not converge") | ||
|
|
||
| dm0 = mf_disp.make_rdm1() | ||
| grad = mf_disp.nuc_grad_method() | ||
| gradient = grad.kernel() | ||
| if hasattr(gradient, "get"): | ||
| gradient = gradient.get() | ||
| force_sets.append(np.asarray(gradient) * GRAD_TO_FORCE) | ||
|
|
||
| del gradient, grad, mf_disp | ||
|
|
||
| self.force_sets = np.asarray(force_sets) | ||
| self.phonon.forces = self.force_sets | ||
| self.phonon.produce_force_constants() | ||
| if self.symmetrize: | ||
| self.phonon.symmetrize_force_constants() | ||
|
|
||
| qpoints = self.phonon.run_qpoints( | ||
| [[0.0, 0.0, 0.0]], | ||
| with_dynamical_matrices=True, | ||
| ) | ||
| dyn_mat = np.asarray(qpoints.dynamical_matrices[0]) | ||
| masses = np.repeat(self.phonon.primitive.masses, 3) | ||
| force_constants = ( | ||
| dyn_mat * np.sqrt(masses[:, None] * masses[None, :]) | ||
| ) | ||
| self.force_constants = np.asarray( | ||
| np.real_if_close(force_constants) * EV_A2_TO_HA_BOHR2, | ||
| dtype=np.float64, | ||
| ) | ||
| return self.force_constants | ||
| finally: | ||
| cell.set_geom_( | ||
|
Collaborator
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. By using inplace=False above, restoring original geometry is not needed |
||
| original_atom, | ||
| a=original_lattice, | ||
| unit=original_unit, | ||
| ) | ||
|
|
||
| def phonon_modes(self, unit="cm-1"): | ||
| """Diagonalize the Gamma dynamical matrix manually. | ||
|
|
||
| Returns frequencies, mass-weighted eigenvectors, and the dynamical | ||
| matrix in atomic units. | ||
| """ | ||
| if self.force_constants is None: | ||
| raise RuntimeError("kernel() must be called before phonon_modes()") | ||
|
|
||
| fc = np.asarray(self.force_constants, dtype=np.float64) | ||
| masses_amu = np.asarray( | ||
| self.phonon.primitive.masses, | ||
| dtype=np.float64, | ||
| ) | ||
| size = 3 * len(masses_amu) | ||
| if fc.shape != (size, size): | ||
| raise ValueError( | ||
| f"force_constants must have shape ({size}, {size}); " | ||
| f"received {fc.shape}" | ||
| ) | ||
|
|
||
| unit_key = self._validate_frequency_unit(unit) | ||
| masses_me = masses_amu * AMU2AU | ||
| mass_inv_sqrt = 1.0 / np.sqrt(np.repeat(masses_me, 3)) | ||
| dyn_mat = fc * mass_inv_sqrt[:, None] * mass_inv_sqrt[None, :] | ||
| eigenvalues, eigenvectors = np.linalg.eigh(dyn_mat) | ||
|
|
||
| factor = ( | ||
| HARTREE2WAVENUMBER | ||
| if unit_key == "cm-1" | ||
| else HARTREE_TO_THZ | ||
| ) | ||
| frequencies = np.sign(eigenvalues) * np.sqrt(np.abs(eigenvalues)) | ||
| frequencies *= factor | ||
| self._log_frequencies(frequencies, unit_key, "manually") | ||
| return frequencies, eigenvectors, dyn_mat | ||
|
|
||
| def phonopy_modes(self, unit="cm-1"): | ||
| """Calculate Gamma-point modes through the phonopy q-point API. | ||
|
|
||
| Returns frequencies, mass-weighted eigenvectors, and the dynamical | ||
| matrix in atomic units. | ||
| """ | ||
| if self.phonon is None or self.phonon.force_constants is None: | ||
| raise RuntimeError("kernel() must be called before phonopy_modes()") | ||
|
|
||
| unit_key = self._validate_frequency_unit(unit) | ||
| qpoints = self.phonon.run_qpoints( | ||
| [[0.0, 0.0, 0.0]], | ||
| with_eigenvectors=True, | ||
| with_dynamical_matrices=True, | ||
| ) | ||
| frequencies = np.asarray(qpoints.frequencies[0]).copy() | ||
| if unit_key == "cm-1": | ||
| frequencies *= HARTREE2WAVENUMBER / HARTREE_TO_THZ | ||
|
|
||
| eigenvectors = np.asarray(qpoints.eigenvectors[0]).copy() | ||
| dyn_mat = np.asarray(qpoints.dynamical_matrices[0]).copy() | ||
| dyn_mat *= EV_A2_TO_HA_BOHR2 / AMU2AU | ||
| dyn_mat = np.real_if_close(dyn_mat) | ||
|
|
||
| self._log_frequencies(frequencies, unit_key, "phonopy") | ||
| return frequencies, eigenvectors, dyn_mat | ||
|
|
||
| @staticmethod | ||
| def _validate_frequency_unit(unit): | ||
| unit_key = unit.lower() | ||
| if unit_key not in ("cm-1", "thz"): | ||
| raise ValueError("unit must be 'cm-1' or 'thz'") | ||
| return unit_key | ||
|
|
||
| def _log_frequencies(self, frequencies, unit, source): | ||
| logger.info( | ||
| self.mf, | ||
| "Lowest Gamma-point frequencies from %s (%s): %s", | ||
| source, | ||
| unit, | ||
| np.array2string( | ||
| frequencies[: min(6, frequencies.size)], | ||
| precision=4, | ||
| ), | ||
| ) | ||
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symbols=cell.elements