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| # This file is a part of the `nequip` package. Please see LICENSE and README at the root for information on using it. | |
| from typing import Union, Optional, List | |
| import torch | |
| from e3nn.o3._irreps import Irreps | |
| from e3nn.util.jit import compile_mode | |
| from onescience.datapipes.materials.nequip import AtomicDataDict | |
| from onescience.datapipes.materials.nequip.misc import chemical_symbols_to_atomic_numbers_dict | |
| from ._graph_mixin import GraphModuleMixin | |
| from .utils import scatter, with_edge_vectors_ | |
| from onescience.utils.nequip.internal.compile import conditional_torchscript_jit | |
| from .embedding.cutoffs import PolynomialCutoff | |
| class _LJParam(torch.nn.Module): | |
| def __init__(self): | |
| super().__init__() | |
| def forward(self, param, index1, index2): | |
| if param.ndim == 2: | |
| # make it symmetric | |
| param = param.triu() + param.triu(1).transpose(-1, -2) | |
| # get for each atom pair | |
| param = torch.index_select( | |
| param.view(-1), 0, index1 * param.shape[0] + index2 | |
| ) | |
| # make it positive | |
| param = param.relu() # TODO: better way? | |
| return param | |
| class LennardJones(GraphModuleMixin, torch.nn.Module): | |
| """Lennard-Jones and related pair potentials.""" | |
| lj_style: str | |
| exponent: float | |
| def __init__( | |
| self, | |
| type_names: List[str], | |
| lj_sigma: Union[torch.Tensor, float], | |
| lj_delta: Union[torch.Tensor, float] = 0, | |
| lj_epsilon: Optional[Union[torch.Tensor, float]] = None, | |
| lj_sigma_trainable: bool = False, | |
| lj_delta_trainable: bool = False, | |
| lj_epsilon_trainable: bool = False, | |
| lj_exponent: Optional[float] = None, | |
| lj_per_type: bool = True, | |
| lj_style: str = "lj", | |
| polynomial_cutoff_p: float = 6.0, | |
| per_atom_energy_field: str = AtomicDataDict.PER_ATOM_ENERGY_KEY, | |
| irreps_in=None, | |
| ) -> None: | |
| super().__init__() | |
| num_types = len(type_names) | |
| self.per_atom_energy_field = per_atom_energy_field | |
| # === irreps registration === | |
| self._init_irreps( | |
| irreps_in=irreps_in, | |
| required_irreps_in=[AtomicDataDict.NORM_LENGTH_KEY], | |
| irreps_out={self.per_atom_energy_field: "0e"}, | |
| ) | |
| if self.per_atom_energy_field in self.irreps_in: | |
| energy_irreps = Irreps(self.irreps_in[self.per_atom_energy_field]) | |
| assert all(ir.l == 0 for _, ir in energy_irreps), ( | |
| f"{self.per_atom_energy_field} must be scalar irreps, found {energy_irreps}" | |
| ) | |
| self.irreps_out[self.per_atom_energy_field] = energy_irreps | |
| assert lj_style in ("lj", "lj_repulsive_only", "repulsive") | |
| self.lj_style = lj_style | |
| for param, (value, trainable) in { | |
| "epsilon": (lj_epsilon, lj_epsilon_trainable), | |
| "sigma": (lj_sigma, lj_sigma_trainable), | |
| "delta": (lj_delta, lj_delta_trainable), | |
| }.items(): | |
| if value is None: | |
| self.register_buffer(param, torch.Tensor()) # torchscript | |
| continue | |
| value = torch.as_tensor(value, dtype=torch.get_default_dtype()) | |
| if value.ndim == 0 and lj_per_type: | |
| # one scalar for all pair types | |
| value = ( | |
| torch.ones( | |
| num_types, num_types, device=value.device, dtype=value.dtype | |
| ) | |
| * value | |
| ) | |
| elif value.ndim == 2: | |
| assert lj_per_type | |
| # one per pair type, check symmetric | |
| assert value.shape == (num_types, num_types) | |
| # per-species square, make sure symmetric | |
| assert torch.equal(value, value.T) | |
| value = torch.triu(value) | |
| else: | |
| raise ValueError | |
| setattr(self, param, torch.nn.Parameter(value, requires_grad=trainable)) | |
| if lj_exponent is None: | |
| lj_exponent = 6.0 | |
| self.exponent = lj_exponent | |
| self.cutoff = conditional_torchscript_jit(PolynomialCutoff(polynomial_cutoff_p)) | |
| self.model_dtype = torch.get_default_dtype() | |
| self._param = conditional_torchscript_jit(_LJParam()) | |
| def forward(self, data: AtomicDataDict.Type) -> AtomicDataDict.Type: | |
| data = with_edge_vectors_(data, with_lengths=True) | |
| edge_center = data[AtomicDataDict.EDGE_INDEX_KEY][0] | |
| atom_types = data[AtomicDataDict.ATOM_TYPE_KEY] | |
| edge_len = data[AtomicDataDict.EDGE_LENGTH_KEY].unsqueeze(-1) | |
| edge_types = torch.index_select( | |
| atom_types, 0, data[AtomicDataDict.EDGE_INDEX_KEY].reshape(-1) | |
| ).view(2, -1) | |
| index1 = edge_types[0] | |
| index2 = edge_types[1] | |
| sigma = self._param(self.sigma, index1, index2) | |
| delta = self._param(self.delta, index1, index2) | |
| epsilon = self._param(self.epsilon, index1, index2) | |
| if self.lj_style == "repulsive": | |
| # 0.5 to assign half and half the energy to each side of the interaction | |
| lj_eng = 0.5 * epsilon * ((sigma * (edge_len - delta)) ** -self.exponent) | |
| else: | |
| lj_eng = (sigma / (edge_len - delta)) ** self.exponent | |
| lj_eng = torch.neg(lj_eng) | |
| lj_eng = lj_eng + lj_eng.square() | |
| # 2.0 because we do the slightly symmetric thing and let | |
| # ij and ji each contribute half of the LJ energy of the pair | |
| # this avoids indexing out certain edges in the general case where | |
| # the edges are not ordered. | |
| lj_eng = (2.0 * epsilon) * lj_eng | |
| if self.lj_style == "lj_repulsive_only": | |
| # if taking only the repulsive part, shift up so the minima is at eng=0 | |
| lj_eng = lj_eng + epsilon | |
| # this is continuous at the minima, and we mask out everything greater | |
| # TODO: this is probably broken with NaNs at delta | |
| lj_eng = lj_eng * (edge_len < (2 ** (1.0 / self.exponent) + delta)) | |
| # apply polynomial cutoff from this module's own normalized edge lengths | |
| lj_edge_cutoff = self.cutoff(data[AtomicDataDict.NORM_LENGTH_KEY]).to( | |
| self.model_dtype | |
| ) | |
| lj_eng = lj_eng.to(self.model_dtype) * lj_edge_cutoff | |
| # sum edge LJ energies onto atoms | |
| atomic_eng = scatter( | |
| lj_eng, | |
| edge_center, | |
| dim=0, | |
| dim_size=AtomicDataDict.num_nodes(data), | |
| ) | |
| if self.per_atom_energy_field in data: | |
| atomic_eng = atomic_eng + data[self.per_atom_energy_field] | |
| data[self.per_atom_energy_field] = atomic_eng | |
| return data | |
| def __repr__(self) -> str: | |
| def _f(e): | |
| e = e.data | |
| if e.ndim == 0: | |
| return f"{e:.6f}" | |
| elif e.ndim == 2: | |
| return f"{e}" | |
| return f"PairPotential(lj_style={self.lj_style} | σ={_f(self.sigma)} δ={_f(self.delta)} ε={_f(self.epsilon)} exp={self.exponent:.1f})" | |
| class SimpleLennardJones(GraphModuleMixin, torch.nn.Module): | |
| """Simple Lennard-Jones.""" | |
| lj_sigma: float | |
| lj_epsilon: float | |
| def __init__( | |
| self, | |
| lj_sigma: float, | |
| lj_epsilon: float, | |
| polynomial_cutoff_p: float = 6.0, | |
| irreps_in=None, | |
| ) -> None: | |
| super().__init__() | |
| self._init_irreps( | |
| irreps_in=irreps_in, | |
| required_irreps_in=[AtomicDataDict.NORM_LENGTH_KEY], | |
| irreps_out={AtomicDataDict.PER_ATOM_ENERGY_KEY: "0e"}, | |
| ) | |
| self.lj_sigma = lj_sigma | |
| self.lj_epsilon = lj_epsilon | |
| self.cutoff = conditional_torchscript_jit(PolynomialCutoff(polynomial_cutoff_p)) | |
| self.model_dtype = torch.get_default_dtype() | |
| def forward(self, data: AtomicDataDict.Type) -> AtomicDataDict.Type: | |
| data = with_edge_vectors_(data, with_lengths=True) | |
| edge_center = data[AtomicDataDict.EDGE_INDEX_KEY][0] | |
| edge_len = data[AtomicDataDict.EDGE_LENGTH_KEY].unsqueeze(-1) | |
| lj_eng = (self.lj_sigma / edge_len) ** 6.0 | |
| lj_eng = lj_eng.square() - lj_eng | |
| lj_eng = 2 * self.lj_epsilon * lj_eng | |
| # apply polynomial cutoff from this module's own normalized edge lengths | |
| lj_edge_cutoff = self.cutoff(data[AtomicDataDict.NORM_LENGTH_KEY]).to( | |
| self.model_dtype | |
| ) | |
| lj_eng = lj_eng.to(self.model_dtype) * lj_edge_cutoff | |
| # sum edge LJ energies onto atoms | |
| atomic_eng = scatter( | |
| lj_eng, | |
| edge_center, | |
| dim=0, | |
| dim_size=AtomicDataDict.num_nodes(data), | |
| ) | |
| if AtomicDataDict.PER_ATOM_ENERGY_KEY in data: | |
| atomic_eng = atomic_eng + data[AtomicDataDict.PER_ATOM_ENERGY_KEY] | |
| data[AtomicDataDict.PER_ATOM_ENERGY_KEY] = atomic_eng | |
| return data | |
| class _ZBL(torch.nn.Module): | |
| def __init__(self): | |
| super().__init__() | |
| def forward( | |
| self, | |
| Z: torch.Tensor, | |
| r: torch.Tensor, | |
| atom_types: torch.Tensor, | |
| edge_index: torch.Tensor, | |
| qqr2exesquare: float, | |
| ) -> torch.Tensor: | |
| # from LAMMPS pair_zbl_const.h | |
| pzbl: float = 0.23 | |
| a0: float = 0.46850 | |
| c1: float = 0.02817 | |
| c2: float = 0.28022 | |
| c3: float = 0.50986 | |
| c4: float = 0.18175 | |
| d1: float = -0.20162 | |
| d2: float = -0.40290 | |
| d3: float = -0.94229 | |
| d4: float = -3.19980 | |
| # (num_atoms,) -> (num_atoms, 1) | |
| node_Zs = torch.nn.functional.embedding(atom_types.view(-1), Z.view(-1, 1)) | |
| # (num_atoms,) -> (2 * num_edges,) | |
| edge_Zs = torch.nn.functional.embedding(edge_index.view(-1), node_Zs).view( | |
| 2, -1 | |
| ) | |
| Zi = torch.select(edge_Zs, 0, 0) | |
| Zj = torch.select(edge_Zs, 0, 1) | |
| del node_Zs, edge_Zs | |
| x = ((torch.pow(Zi, pzbl) + torch.pow(Zj, pzbl)) * r) / a0 | |
| psi = ( | |
| c1 * (d1 * x).exp() | |
| + c2 * (d2 * x).exp() | |
| + c3 * (d3 * x).exp() | |
| + c4 * (d4 * x).exp() | |
| ) | |
| eng = qqr2exesquare * ((Zi * Zj) / r) * psi | |
| return eng | |
| class ZBL(GraphModuleMixin, torch.nn.Module): | |
| """`ZBL <https://docs.lammps.org/pair_zbl.html>`_ pair potential energy term. | |
| Useful as a prior for core repulsion to mitigate molecular dynamics failure modes associated with atoms getting too close. | |
| Args: | |
| type_names (List[str]): list of type names known by the model, ``[atom1, atom2, atom3]`` | |
| chemical_species (List[str]): list of chemical symbols, e.g. ``[C, H, O]`` | |
| units (str): `LAMMPS units <https://docs.lammps.org/units.html>`_ that the data is in; ``metal`` and ``real`` are presently supported -- raise a GitHub issue if more is desired | |
| polynomial_cutoff_p (float): exponent used for the polynomial cutoff (default ``6``) | |
| """ | |
| def __init__( | |
| self, | |
| type_names: List[str], | |
| chemical_species: List[str], | |
| units: str, | |
| polynomial_cutoff_p: float = 6.0, | |
| per_atom_energy_field: str = AtomicDataDict.PER_ATOM_ENERGY_KEY, | |
| irreps_in=None, | |
| ): | |
| super().__init__() | |
| num_types = len(type_names) | |
| self.per_atom_energy_field = per_atom_energy_field | |
| # === irreps registration === | |
| self._init_irreps( | |
| irreps_in=irreps_in, | |
| required_irreps_in=[AtomicDataDict.NORM_LENGTH_KEY], | |
| irreps_out={self.per_atom_energy_field: "0e"}, | |
| ) | |
| if self.per_atom_energy_field in self.irreps_in: | |
| energy_irreps = Irreps(self.irreps_in[self.per_atom_energy_field]) | |
| assert all(ir.l == 0 for _, ir in energy_irreps), ( | |
| f"{self.per_atom_energy_field} must be scalar irreps, found {energy_irreps}" | |
| ) | |
| self.irreps_out[self.per_atom_energy_field] = energy_irreps | |
| assert len(chemical_species) == num_types | |
| atomic_numbers: List[int] = [ | |
| chemical_symbols_to_atomic_numbers_dict[chemical_species[type_i]] | |
| for type_i in range(num_types) | |
| ] | |
| if min(atomic_numbers) < 1: | |
| raise ValueError( | |
| f"Your chemical symbols don't seem valid (minimum atomic number is {min(atomic_numbers)} < 1); did you try to use fake chemical symbols for arbitrary atom types?" | |
| ) | |
| # LAMMPS note on units: | |
| # > The numerical values of the exponential decay constants in the | |
| # > screening function depend on the unit of distance. In the above | |
| # > equation they are given for units of Angstroms. LAMMPS will | |
| # > automatically convert these values to the distance unit of the | |
| # > specified LAMMPS units setting. The values of Z should always be | |
| # > given as multiples of a proton’s charge, e.g. 29.0 for copper. | |
| # So, we store the atomic numbers directly. | |
| self.register_buffer( | |
| "atomic_numbers", | |
| torch.as_tensor(atomic_numbers, dtype=torch.get_default_dtype()), | |
| ) | |
| # And we have to convert our value of prefector into the model's physical units | |
| # Here, prefactor is (electron charge)^2 / (4 * pi * electrical permisivity of vacuum) | |
| # we have a value for that in eV and Angstrom | |
| # See https://github.com/lammps/lammps/blob/c415385ab4b0983fa1c72f9e92a09a8ed7eebe4a/src/update.cpp#L187 for values from LAMMPS | |
| # LAMMPS uses `force->qqr2e * force->qelectron * force->qelectron` | |
| # Make it a buffer so rescalings are persistent, it still acts as a scalar Tensor | |
| self.register_buffer( | |
| "_qqr2exesquare", | |
| torch.as_tensor( | |
| {"metal": 14.399645 * (1.0) ** 2, "real": 332.06371 * (1.0) ** 2}[ | |
| units | |
| ], | |
| dtype=torch.float64, | |
| ) | |
| * 0.5, # Put half the energy on each of ij, ji | |
| ) | |
| self.cutoff = conditional_torchscript_jit(PolynomialCutoff(polynomial_cutoff_p)) | |
| self.model_dtype = torch.get_default_dtype() | |
| self._zbl = conditional_torchscript_jit(_ZBL()) | |
| def forward(self, data: AtomicDataDict.Type) -> AtomicDataDict.Type: | |
| """""" | |
| data = with_edge_vectors_(data, with_lengths=True) | |
| edge_center = data[AtomicDataDict.EDGE_INDEX_KEY][0] | |
| # account for possibility of reduced num nodes in atomic energy in a local-ghost atom context | |
| if self.per_atom_energy_field in data: | |
| num_nodes = data[self.per_atom_energy_field].size(0) | |
| else: | |
| num_nodes = AtomicDataDict.num_nodes(data) | |
| zbl_edge_eng = self._zbl( | |
| Z=self.atomic_numbers, | |
| r=data[AtomicDataDict.EDGE_LENGTH_KEY].view(-1), | |
| atom_types=data[AtomicDataDict.ATOM_TYPE_KEY], | |
| edge_index=data[AtomicDataDict.EDGE_INDEX_KEY], | |
| qqr2exesquare=self._qqr2exesquare, | |
| ).unsqueeze(-1) | |
| # apply cutoff | |
| zbl_edge_cutoff = self.cutoff(data[AtomicDataDict.NORM_LENGTH_KEY]).to( | |
| self.model_dtype | |
| ) | |
| zbl_edge_eng = zbl_edge_eng * zbl_edge_cutoff | |
| atomic_eng = scatter( | |
| zbl_edge_eng, | |
| edge_center, | |
| dim=0, | |
| dim_size=num_nodes, | |
| ) | |
| if self.per_atom_energy_field in data: | |
| atomic_eng = atomic_eng + data[self.per_atom_energy_field] | |
| data[self.per_atom_energy_field] = atomic_eng | |
| return data | |
| __all__ = [LennardJones, ZBL] | |