153 lines
4.6 KiB
Python
153 lines
4.6 KiB
Python
import torch
|
|
import torch.nn as nn
|
|
from modules.activations import swish
|
|
from modules.bessel_basis_layer import BesselBasisLayer
|
|
from modules.embedding_block import EmbeddingBlock
|
|
from modules.interaction_block import InteractionBlock
|
|
from modules.output_block import OutputBlock
|
|
from modules.spherical_basis_layer import SphericalBasisLayer
|
|
|
|
|
|
class DimeNet(nn.Module):
|
|
"""
|
|
DimeNet model.
|
|
|
|
Parameters
|
|
----------
|
|
emb_size
|
|
Embedding size used throughout the model
|
|
num_blocks
|
|
Number of building blocks to be stacked
|
|
num_bilinear
|
|
Third dimension of the bilinear layer tensor
|
|
num_spherical
|
|
Number of spherical harmonics
|
|
num_radial
|
|
Number of radial basis functions
|
|
cutoff
|
|
Cutoff distance for interatomic interactions
|
|
envelope_exponent
|
|
Shape of the smooth cutoff
|
|
num_before_skip
|
|
Number of residual layers in interaction block before skip connection
|
|
num_after_skip
|
|
Number of residual layers in interaction block after skip connection
|
|
num_dense_output
|
|
Number of dense layers for the output blocks
|
|
num_targets
|
|
Number of targets to predict
|
|
activation
|
|
Activation function
|
|
output_init
|
|
Initial function in output block
|
|
"""
|
|
|
|
def __init__(
|
|
self,
|
|
emb_size,
|
|
num_blocks,
|
|
num_bilinear,
|
|
num_spherical,
|
|
num_radial,
|
|
cutoff=5.0,
|
|
envelope_exponent=5,
|
|
num_before_skip=1,
|
|
num_after_skip=2,
|
|
num_dense_output=3,
|
|
num_targets=12,
|
|
activation=swish,
|
|
output_init=nn.init.zeros_,
|
|
):
|
|
super(DimeNet, self).__init__()
|
|
|
|
self.num_blocks = num_blocks
|
|
self.num_radial = num_radial
|
|
|
|
# cosine basis function expansion layer
|
|
self.rbf_layer = BesselBasisLayer(
|
|
num_radial=num_radial,
|
|
cutoff=cutoff,
|
|
envelope_exponent=envelope_exponent,
|
|
)
|
|
|
|
self.sbf_layer = SphericalBasisLayer(
|
|
num_spherical=num_spherical,
|
|
num_radial=num_radial,
|
|
cutoff=cutoff,
|
|
envelope_exponent=envelope_exponent,
|
|
)
|
|
|
|
# embedding block
|
|
self.emb_block = EmbeddingBlock(
|
|
emb_size=emb_size,
|
|
num_radial=num_radial,
|
|
bessel_funcs=self.sbf_layer.get_bessel_funcs(),
|
|
cutoff=cutoff,
|
|
envelope_exponent=envelope_exponent,
|
|
activation=activation,
|
|
)
|
|
|
|
# output block
|
|
self.output_blocks = nn.ModuleList(
|
|
{
|
|
OutputBlock(
|
|
emb_size=emb_size,
|
|
num_radial=num_radial,
|
|
num_dense=num_dense_output,
|
|
num_targets=num_targets,
|
|
activation=activation,
|
|
output_init=output_init,
|
|
)
|
|
for _ in range(num_blocks + 1)
|
|
}
|
|
)
|
|
|
|
# interaction block
|
|
self.interaction_blocks = nn.ModuleList(
|
|
{
|
|
InteractionBlock(
|
|
emb_size=emb_size,
|
|
num_radial=num_radial,
|
|
num_spherical=num_spherical,
|
|
num_bilinear=num_bilinear,
|
|
num_before_skip=num_before_skip,
|
|
num_after_skip=num_after_skip,
|
|
activation=activation,
|
|
)
|
|
for _ in range(num_blocks)
|
|
}
|
|
)
|
|
|
|
def edge_init(self, edges):
|
|
# Calculate angles k -> j -> i
|
|
R1, R2 = edges.src["o"], edges.dst["o"]
|
|
x = torch.sum(R1 * R2, dim=-1)
|
|
y = torch.cross(R1, R2)
|
|
y = torch.norm(y, dim=-1)
|
|
angle = torch.atan2(y, x)
|
|
# Transform via angles
|
|
cbf = [f(angle) for f in self.sbf_layer.get_sph_funcs()]
|
|
cbf = torch.stack(cbf, dim=1) # [None, 7]
|
|
cbf = cbf.repeat_interleave(self.num_radial, dim=1) # [None, 42]
|
|
sbf = edges.src["rbf_env"] * cbf # [None, 42]
|
|
return {"sbf": sbf}
|
|
|
|
def forward(self, g, l_g):
|
|
# add rbf features for each edge in one batch graph, [num_radial,]
|
|
g = self.rbf_layer(g)
|
|
# Embedding block
|
|
g = self.emb_block(g)
|
|
# Output block
|
|
P = self.output_blocks[0](g) # [batch_size, num_targets]
|
|
# Prepare sbf feature before the following blocks
|
|
for k, v in g.edata.items():
|
|
l_g.ndata[k] = v
|
|
|
|
l_g.apply_edges(self.edge_init)
|
|
# Interaction blocks
|
|
for i in range(self.num_blocks):
|
|
g = self.interaction_blocks[i](g, l_g)
|
|
P += self.output_blocks[i + 1](g)
|
|
|
|
return P
|