File size: 8,154 Bytes
f555e1d
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
208
209
210
211
212
213
214
215
216
217
218
219
220
221
222
223
224
225
226
227
228
229
230
231
232
233
234
235
import numpy as np
import torch
import torch.nn as nn
import torch.nn.functional as F
from torch_scatter import scatter_mean 

# auxiliary function for diffusion
def cosine_beta_schedule(timesteps, s=0.008):
    """
    cosine schedule
    as proposed in https://openreview.net/forum?id=-NEXDKk8gZ
    """
    steps = timesteps + 1
    x = np.linspace(0, steps, steps)
    alphas_cumprod = np.cos(((x / steps) + s) / (1 + s) * np.pi * 0.5) ** 2
    alphas_cumprod = alphas_cumprod / alphas_cumprod[0]
    alphas = (alphas_cumprod[1:] / alphas_cumprod[:-1])

    alphas = np.clip(alphas, a_min=0.001, a_max=1.)

    # Use sqrt of this, so the alpha in our paper is the alpha_sqrt from the
    # Gaussian diffusion in Ho et al.
    alphas = np.sqrt(alphas)
    return alphas



def get_beta_schedule(beta_schedule, *, beta_start, beta_end, num_diffusion_timesteps):
    def sigmoid(x):
        return 1 / (np.exp(-x) + 1)

    if beta_schedule == "quad":
        betas = (
                np.linspace(
                    beta_start ** 0.5,
                    beta_end ** 0.5,
                    num_diffusion_timesteps,
                    dtype=np.float64,
                )
                ** 2
        )
    elif beta_schedule == "linear":
        betas = np.linspace(
            beta_start, beta_end, num_diffusion_timesteps, dtype=np.float64
        )
    elif beta_schedule == "const":
        betas = beta_end * np.ones(num_diffusion_timesteps, dtype=np.float64)
    elif beta_schedule == "jsd":  # 1/T, 1/(T-1), 1/(T-2), ..., 1
        betas = 1.0 / np.linspace(
            num_diffusion_timesteps, 1, num_diffusion_timesteps, dtype=np.float64
        )
    elif beta_schedule == "sigmoid":
        betas = np.linspace(-6, 6, num_diffusion_timesteps)
        betas = sigmoid(betas) * (beta_end - beta_start) + beta_start
    else:
        raise NotImplementedError(beta_schedule)
    assert betas.shape == (num_diffusion_timesteps,)
    return betas


def to_torch_const(x):
    x = torch.from_numpy(x).float()
    x = nn.Parameter(x, requires_grad=False)
    return x

def extract(coef, t, batch):
    out = coef[t][batch]
    return out.unsqueeze(-1)

def log_add_exp(a, b):
    maximum = torch.max(a, b)
    return maximum + torch.log(torch.exp(a - maximum) + torch.exp(b - maximum))

def log_categorical(log_x_start, log_prob):
    return (log_x_start.exp() * log_prob).sum(dim=1)

def categorical_kl(log_prob1, log_prob2):
    kl = (log_prob1.exp() * (log_prob1 - log_prob2)).sum(dim=1)
    return kl


def log_sample_categorical(logits):
    uniform = torch.rand_like(logits)
    gumbel_noise = -torch.log(-torch.log(uniform + 1e-30) + 1e-30)
    sample_index = (gumbel_noise + logits).argmax(dim=-1)
    return sample_index


def index_to_log_onehot(x, num_classes):
    assert x.max().item() < num_classes, f'Error: {x.max().item()} >= {num_classes}'
    x_onehot = F.one_hot(x, num_classes)
    # permute_order = (0, -1) + tuple(range(1, len(x.size())))
    # x_onehot = x_onehot.permute(permute_order)
    log_x = torch.log(x_onehot.float().clamp(min=1e-30))
    return log_x

def log_1_min_a(a):
    return np.log(1 - np.exp(a) + 1e-40)

def q_v_pred(log_v0, t, log_alphas_cumprod_v, log_one_minus_alphas_cumprod_v, batch):
    # compute q(vt | v0)
    log_cumprod_alpha_t = extract(log_alphas_cumprod_v, t, batch)
    log_1_min_cumprod_alpha = extract(log_one_minus_alphas_cumprod_v, t, batch)

    log_probs = log_add_exp(
        log_v0 + log_cumprod_alpha_t,
        log_1_min_cumprod_alpha - np.log(30)
    )
    return log_probs

def q_v_sample(log_v0, log_alphas_cumprod_v, log_one_minus_alphas_cumprod_v, t, batch):
        log_qvt_v0 = q_v_pred(log_v0, t, log_alphas_cumprod_v, log_one_minus_alphas_cumprod_v, batch)
        sample_index = log_sample_categorical(log_qvt_v0)
        log_sample = index_to_log_onehot(sample_index, 30)
        return sample_index, log_sample

def sample_time(num_graphs, num_timesteps, device, method='symmetric', low_ratio=0.3):
    if method == 'symmetric':
        time_step = torch.randint(
            0, num_timesteps, size=(num_graphs // 2 + 1,), device=device)
        time_step = torch.cat(
            [time_step, num_timesteps - time_step - 1], dim=0)[:num_graphs]
        pt = torch.ones_like(time_step).float() / num_timesteps
        return time_step, pt
    elif method == 'mid_symmetric':
        # only use mid timesteps, i.e., [300,700]
        t_min = int(num_timesteps * low_ratio)
        t_max = num_timesteps - t_min 
        time_step = torch.randint(
            t_min, t_max, size=(num_graphs // 2 + 1,), device=device)
        time_step = torch.cat(
            [time_step, num_timesteps - time_step - 1], dim=0)[:num_graphs]
        pt = torch.ones_like(time_step).float() / (t_max - t_min)
        return time_step, pt

    else:
        raise ValueError


def compute_v_Lt(log_v_model_prob, log_v0, log_v_true_prob, t, batch):
    kl_v = categorical_kl(log_v_true_prob, log_v_model_prob)  # [num_atoms, ]
    decoder_nll_v = -log_categorical(log_v0, log_v_model_prob)  # L0
    assert kl_v.shape == decoder_nll_v.shape
    mask = (t == 0).float()[batch]
    loss_v = scatter_mean(mask * decoder_nll_v + (1. - mask) * kl_v, batch, dim=0)
    return loss_v


# atom type diffusion process
def q_v_pred_one_timestep(log_vt_1, t, log_alphas_v, log_one_minus_alphas_v, batch):
    # q(vt | vt-1)
    log_alpha_t = extract(log_alphas_v, t, batch)
    log_1_min_alpha_t = extract(log_one_minus_alphas_v, t, batch)

    # alpha_t * vt + (1 - alpha_t) 1 / K
    log_probs = log_add_exp(
        log_vt_1 + log_alpha_t,
        log_1_min_alpha_t - np.log(30)
    )
    return log_probs

 # atom type generative process
def q_v_posterior(log_v0, log_vt, log_alphas_cumprod_v, log_one_minus_alphas_cumprod_v, log_alphas_v, log_one_minus_alphas_v, t, batch):
    # q(vt-1 | vt, v0) = q(vt | vt-1, x0) * q(vt-1 | x0) / q(vt | x0)
    t_minus_1 = t - 1
    # Remove negative values, will not be used anyway for final decoder
    t_minus_1 = torch.where(t_minus_1 < 0, torch.zeros_like(t_minus_1), t_minus_1)
    log_qvt1_v0 = q_v_pred(log_v0, t_minus_1,  log_alphas_cumprod_v, log_one_minus_alphas_cumprod_v, batch)
    unnormed_logprobs = log_qvt1_v0 + q_v_pred_one_timestep(log_vt, t, log_alphas_v, log_one_minus_alphas_v, batch)
    log_vt1_given_vt_v0 = unnormed_logprobs - torch.logsumexp(unnormed_logprobs, dim=-1, keepdim=True)
    return log_vt1_given_vt_v0

def diffusion_loss(
    ligand_pos,           
    ligand_pos_perturbed, 
    pred_ligand_pos,     
    pred_ligand_v,      
    log_ligand_v0,       
    log_ligand_vt,    

    log_alphas_cumprod_v, 
    log_one_minus_alphas_cumprod_v, 
    log_alphas_v, 
    log_one_minus_alphas_v,
    
    time_step,        
    batch_ligand 
):
    ## using FP32 to prevent NAN/INF and then cast back to FP16
    target_pos = ligand_pos.float()
    pred_pos   = pred_ligand_pos.float()

    per_atom_pos_mse = ((pred_pos - target_pos) ** 2).sum(-1)
    loss_pos = scatter_mean(per_atom_pos_mse, batch_ligand, dim=0).mean()

    logits_v = pred_ligand_v.float()
    log_v_recon = F.log_softmax(logits_v, dim=-1)

    log_v0 = log_ligand_v0.float()
    log_vt = log_ligand_vt.float()

    log_v_model_prob = q_v_posterior(
        log_v_recon,
        log_vt,
        log_alphas_cumprod_v.float(),
        log_one_minus_alphas_cumprod_v.float(),
        log_alphas_v.float(),
        log_one_minus_alphas_v.float(),
        time_step,
        batch_ligand,
    )
    log_v_true_prob = q_v_posterior(
        log_v0,
        log_vt,
        log_alphas_cumprod_v.float(),
        log_one_minus_alphas_cumprod_v.float(),
        log_alphas_v.float(),
        log_one_minus_alphas_v.float(),
        time_step,
        batch_ligand,
    )

    kl_v = compute_v_Lt(
        log_v_model_prob=log_v_model_prob,
        log_v0=log_v0,                      
        log_v_true_prob=log_v_true_prob,
        t=time_step,
        batch=batch_ligand,
    )
    loss_v = kl_v.mean()

    loss = loss_pos + 100 * loss_v

    return (loss.to(pred_ligand_pos.dtype), loss_pos.to(pred_ligand_pos.dtype), loss_v.to(pred_ligand_pos.dtype))