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import torch |
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import torch.nn.functional as F |
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import math |
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from tqdm import tqdm |
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|
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class NoiseScheduleVP: |
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def __init__( |
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self, |
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schedule='discrete', |
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betas=None, |
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alphas_cumprod=None, |
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continuous_beta_0=0.1, |
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continuous_beta_1=20., |
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): |
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"""Create a wrapper class for the forward SDE (VP type). |
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*** |
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Update: We support discrete-time diffusion models by implementing a picewise linear interpolation for log_alpha_t. |
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We recommend to use schedule='discrete' for the discrete-time diffusion models, especially for high-resolution images. |
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*** |
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The forward SDE ensures that the condition distribution q_{t|0}(x_t | x_0) = N ( alpha_t * x_0, sigma_t^2 * I ). |
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We further define lambda_t = log(alpha_t) - log(sigma_t), which is the half-logSNR (described in the DPM-Solver paper). |
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Therefore, we implement the functions for computing alpha_t, sigma_t and lambda_t. For t in [0, T], we have: |
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log_alpha_t = self.marginal_log_mean_coeff(t) |
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sigma_t = self.marginal_std(t) |
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lambda_t = self.marginal_lambda(t) |
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Moreover, as lambda(t) is an invertible function, we also support its inverse function: |
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t = self.inverse_lambda(lambda_t) |
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=============================================================== |
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We support both discrete-time DPMs (trained on n = 0, 1, ..., N-1) and continuous-time DPMs (trained on t in [t_0, T]). |
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1. For discrete-time DPMs: |
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For discrete-time DPMs trained on n = 0, 1, ..., N-1, we convert the discrete steps to continuous time steps by: |
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t_i = (i + 1) / N |
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e.g. for N = 1000, we have t_0 = 1e-3 and T = t_{N-1} = 1. |
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We solve the corresponding diffusion ODE from time T = 1 to time t_0 = 1e-3. |
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Args: |
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betas: A `torch.Tensor`. The beta array for the discrete-time DPM. (See the original DDPM paper for details) |
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alphas_cumprod: A `torch.Tensor`. The cumprod alphas for the discrete-time DPM. (See the original DDPM paper for details) |
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Note that we always have alphas_cumprod = cumprod(betas). Therefore, we only need to set one of `betas` and `alphas_cumprod`. |
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**Important**: Please pay special attention for the args for `alphas_cumprod`: |
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The `alphas_cumprod` is the \hat{alpha_n} arrays in the notations of DDPM. Specifically, DDPMs assume that |
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q_{t_n | 0}(x_{t_n} | x_0) = N ( \sqrt{\hat{alpha_n}} * x_0, (1 - \hat{alpha_n}) * I ). |
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Therefore, the notation \hat{alpha_n} is different from the notation alpha_t in DPM-Solver. In fact, we have |
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alpha_{t_n} = \sqrt{\hat{alpha_n}}, |
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and |
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log(alpha_{t_n}) = 0.5 * log(\hat{alpha_n}). |
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2. For continuous-time DPMs: |
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We support two types of VPSDEs: linear (DDPM) and cosine (improved-DDPM). The hyperparameters for the noise |
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schedule are the default settings in DDPM and improved-DDPM: |
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Args: |
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beta_min: A `float` number. The smallest beta for the linear schedule. |
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beta_max: A `float` number. The largest beta for the linear schedule. |
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cosine_s: A `float` number. The hyperparameter in the cosine schedule. |
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cosine_beta_max: A `float` number. The hyperparameter in the cosine schedule. |
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T: A `float` number. The ending time of the forward process. |
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=============================================================== |
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Args: |
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schedule: A `str`. The noise schedule of the forward SDE. 'discrete' for discrete-time DPMs, |
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'linear' or 'cosine' for continuous-time DPMs. |
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Returns: |
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A wrapper object of the forward SDE (VP type). |
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|
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=============================================================== |
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Example: |
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# For discrete-time DPMs, given betas (the beta array for n = 0, 1, ..., N - 1): |
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>>> ns = NoiseScheduleVP('discrete', betas=betas) |
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# For discrete-time DPMs, given alphas_cumprod (the \hat{alpha_n} array for n = 0, 1, ..., N - 1): |
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>>> ns = NoiseScheduleVP('discrete', alphas_cumprod=alphas_cumprod) |
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# For continuous-time DPMs (VPSDE), linear schedule: |
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>>> ns = NoiseScheduleVP('linear', continuous_beta_0=0.1, continuous_beta_1=20.) |
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""" |
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if schedule not in ['discrete', 'linear', 'cosine']: |
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raise ValueError( |
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"Unsupported noise schedule {}. The schedule needs to be 'discrete' or 'linear' or 'cosine'".format( |
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schedule)) |
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|
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self.schedule = schedule |
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if schedule == 'discrete': |
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if betas is not None: |
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log_alphas = 0.5 * torch.log(1 - betas).cumsum(dim=0) |
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else: |
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assert alphas_cumprod is not None |
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log_alphas = 0.5 * torch.log(alphas_cumprod) |
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self.total_N = len(log_alphas) |
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self.T = 1. |
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self.t_array = torch.linspace(0., 1., self.total_N + 1)[1:].reshape((1, -1)) |
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self.log_alpha_array = log_alphas.reshape((1, -1,)) |
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else: |
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self.total_N = 1000 |
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self.beta_0 = continuous_beta_0 |
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self.beta_1 = continuous_beta_1 |
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self.cosine_s = 0.008 |
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self.cosine_beta_max = 999. |
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self.cosine_t_max = math.atan(self.cosine_beta_max * (1. + self.cosine_s) / math.pi) * 2. * ( |
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1. + self.cosine_s) / math.pi - self.cosine_s |
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self.cosine_log_alpha_0 = math.log(math.cos(self.cosine_s / (1. + self.cosine_s) * math.pi / 2.)) |
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self.schedule = schedule |
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if schedule == 'cosine': |
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self.T = 0.9946 |
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else: |
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self.T = 1. |
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|
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def marginal_log_mean_coeff(self, t): |
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""" |
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Compute log(alpha_t) of a given continuous-time label t in [0, T]. |
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""" |
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if self.schedule == 'discrete': |
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return interpolate_fn(t.reshape((-1, 1)), self.t_array.to(t.device), |
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self.log_alpha_array.to(t.device)).reshape((-1)) |
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elif self.schedule == 'linear': |
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return -0.25 * t ** 2 * (self.beta_1 - self.beta_0) - 0.5 * t * self.beta_0 |
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elif self.schedule == 'cosine': |
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log_alpha_fn = lambda s: torch.log(torch.cos((s + self.cosine_s) / (1. + self.cosine_s) * math.pi / 2.)) |
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log_alpha_t = log_alpha_fn(t) - self.cosine_log_alpha_0 |
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return log_alpha_t |
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|
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def marginal_alpha(self, t): |
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""" |
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Compute alpha_t of a given continuous-time label t in [0, T]. |
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""" |
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return torch.exp(self.marginal_log_mean_coeff(t)) |
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|
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def marginal_std(self, t): |
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""" |
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Compute sigma_t of a given continuous-time label t in [0, T]. |
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""" |
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return torch.sqrt(1. - torch.exp(2. * self.marginal_log_mean_coeff(t))) |
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|
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def marginal_lambda(self, t): |
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""" |
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Compute lambda_t = log(alpha_t) - log(sigma_t) of a given continuous-time label t in [0, T]. |
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""" |
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log_mean_coeff = self.marginal_log_mean_coeff(t) |
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log_std = 0.5 * torch.log(1. - torch.exp(2. * log_mean_coeff)) |
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return log_mean_coeff - log_std |
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|
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def inverse_lambda(self, lamb): |
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""" |
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Compute the continuous-time label t in [0, T] of a given half-logSNR lambda_t. |
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""" |
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if self.schedule == 'linear': |
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tmp = 2. * (self.beta_1 - self.beta_0) * torch.logaddexp(-2. * lamb, torch.zeros((1,)).to(lamb)) |
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Delta = self.beta_0 ** 2 + tmp |
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return tmp / (torch.sqrt(Delta) + self.beta_0) / (self.beta_1 - self.beta_0) |
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elif self.schedule == 'discrete': |
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log_alpha = -0.5 * torch.logaddexp(torch.zeros((1,)).to(lamb.device), -2. * lamb) |
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t = interpolate_fn(log_alpha.reshape((-1, 1)), torch.flip(self.log_alpha_array.to(lamb.device), [1]), |
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torch.flip(self.t_array.to(lamb.device), [1])) |
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return t.reshape((-1,)) |
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else: |
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log_alpha = -0.5 * torch.logaddexp(-2. * lamb, torch.zeros((1,)).to(lamb)) |
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t_fn = lambda log_alpha_t: torch.arccos(torch.exp(log_alpha_t + self.cosine_log_alpha_0)) * 2. * ( |
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1. + self.cosine_s) / math.pi - self.cosine_s |
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t = t_fn(log_alpha) |
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return t |
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def model_wrapper( |
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model, |
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noise_schedule, |
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model_type="noise", |
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model_kwargs={}, |
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guidance_type="uncond", |
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condition=None, |
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unconditional_condition=None, |
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guidance_scale=1., |
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classifier_fn=None, |
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classifier_kwargs={}, |
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): |
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"""Create a wrapper function for the noise prediction model. |
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DPM-Solver needs to solve the continuous-time diffusion ODEs. For DPMs trained on discrete-time labels, we need to |
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firstly wrap the model function to a noise prediction model that accepts the continuous time as the input. |
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We support four types of the diffusion model by setting `model_type`: |
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1. "noise": noise prediction model. (Trained by predicting noise). |
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2. "x_start": data prediction model. (Trained by predicting the data x_0 at time 0). |
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3. "v": velocity prediction model. (Trained by predicting the velocity). |
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The "v" prediction is derivation detailed in Appendix D of [1], and is used in Imagen-Video [2]. |
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[1] Salimans, Tim, and Jonathan Ho. "Progressive distillation for fast sampling of diffusion models." |
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arXiv preprint arXiv:2202.00512 (2022). |
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[2] Ho, Jonathan, et al. "Imagen Video: High Definition Video Generation with Diffusion Models." |
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arXiv preprint arXiv:2210.02303 (2022). |
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|
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4. "score": marginal score function. (Trained by denoising score matching). |
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Note that the score function and the noise prediction model follows a simple relationship: |
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``` |
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noise(x_t, t) = -sigma_t * score(x_t, t) |
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``` |
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We support three types of guided sampling by DPMs by setting `guidance_type`: |
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1. "uncond": unconditional sampling by DPMs. |
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The input `model` has the following format: |
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`` |
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model(x, t_input, **model_kwargs) -> noise | x_start | v | score |
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`` |
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2. "classifier": classifier guidance sampling [3] by DPMs and another classifier. |
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The input `model` has the following format: |
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`` |
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model(x, t_input, **model_kwargs) -> noise | x_start | v | score |
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`` |
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The input `classifier_fn` has the following format: |
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`` |
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classifier_fn(x, t_input, cond, **classifier_kwargs) -> logits(x, t_input, cond) |
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`` |
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[3] P. Dhariwal and A. Q. Nichol, "Diffusion models beat GANs on image synthesis," |
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in Advances in Neural Information Processing Systems, vol. 34, 2021, pp. 8780-8794. |
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3. "classifier-free": classifier-free guidance sampling by conditional DPMs. |
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The input `model` has the following format: |
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`` |
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model(x, t_input, cond, **model_kwargs) -> noise | x_start | v | score |
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`` |
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And if cond == `unconditional_condition`, the model output is the unconditional DPM output. |
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[4] Ho, Jonathan, and Tim Salimans. "Classifier-free diffusion guidance." |
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arXiv preprint arXiv:2207.12598 (2022). |
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|
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The `t_input` is the time label of the model, which may be discrete-time labels (i.e. 0 to 999) |
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or continuous-time labels (i.e. epsilon to T). |
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We wrap the model function to accept only `x` and `t_continuous` as inputs, and outputs the predicted noise: |
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`` |
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def model_fn(x, t_continuous) -> noise: |
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t_input = get_model_input_time(t_continuous) |
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return noise_pred(model, x, t_input, **model_kwargs) |
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`` |
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where `t_continuous` is the continuous time labels (i.e. epsilon to T). And we use `model_fn` for DPM-Solver. |
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=============================================================== |
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Args: |
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model: A diffusion model with the corresponding format described above. |
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noise_schedule: A noise schedule object, such as NoiseScheduleVP. |
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model_type: A `str`. The parameterization type of the diffusion model. |
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"noise" or "x_start" or "v" or "score". |
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model_kwargs: A `dict`. A dict for the other inputs of the model function. |
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guidance_type: A `str`. The type of the guidance for sampling. |
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"uncond" or "classifier" or "classifier-free". |
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condition: A pytorch tensor. The condition for the guided sampling. |
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Only used for "classifier" or "classifier-free" guidance type. |
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unconditional_condition: A pytorch tensor. The condition for the unconditional sampling. |
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Only used for "classifier-free" guidance type. |
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guidance_scale: A `float`. The scale for the guided sampling. |
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classifier_fn: A classifier function. Only used for the classifier guidance. |
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classifier_kwargs: A `dict`. A dict for the other inputs of the classifier function. |
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Returns: |
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A noise prediction model that accepts the noised data and the continuous time as the inputs. |
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""" |
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|
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def get_model_input_time(t_continuous): |
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""" |
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Convert the continuous-time `t_continuous` (in [epsilon, T]) to the model input time. |
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For discrete-time DPMs, we convert `t_continuous` in [1 / N, 1] to `t_input` in [0, 1000 * (N - 1) / N]. |
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For continuous-time DPMs, we just use `t_continuous`. |
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""" |
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if noise_schedule.schedule == 'discrete': |
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return (t_continuous - 1. / noise_schedule.total_N) * 1000. |
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else: |
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return t_continuous |
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|
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def noise_pred_fn(x, t_continuous, cond=None): |
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if t_continuous.reshape((-1,)).shape[0] == 1: |
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t_continuous = t_continuous.expand((x.shape[0])) |
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t_input = get_model_input_time(t_continuous) |
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if cond is None: |
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output = model(x, t_input, **model_kwargs) |
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else: |
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output = model(x, t_input, cond, **model_kwargs) |
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if model_type == "noise": |
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return output |
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elif model_type == "x_start": |
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alpha_t, sigma_t = noise_schedule.marginal_alpha(t_continuous), noise_schedule.marginal_std(t_continuous) |
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dims = x.dim() |
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return (x - expand_dims(alpha_t, dims) * output) / expand_dims(sigma_t, dims) |
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elif model_type == "v": |
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alpha_t, sigma_t = noise_schedule.marginal_alpha(t_continuous), noise_schedule.marginal_std(t_continuous) |
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dims = x.dim() |
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return expand_dims(alpha_t, dims) * output + expand_dims(sigma_t, dims) * x |
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elif model_type == "score": |
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sigma_t = noise_schedule.marginal_std(t_continuous) |
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dims = x.dim() |
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return -expand_dims(sigma_t, dims) * output |
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|
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def cond_grad_fn(x, t_input): |
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""" |
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Compute the gradient of the classifier, i.e. nabla_{x} log p_t(cond | x_t). |
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""" |
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with torch.enable_grad(): |
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x_in = x.detach().requires_grad_(True) |
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log_prob = classifier_fn(x_in, t_input, condition, **classifier_kwargs) |
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return torch.autograd.grad(log_prob.sum(), x_in)[0] |
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|
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def model_fn(x, t_continuous): |
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""" |
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The noise predicition model function that is used for DPM-Solver. |
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""" |
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if t_continuous.reshape((-1,)).shape[0] == 1: |
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t_continuous = t_continuous.expand((x.shape[0])) |
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if guidance_type == "uncond": |
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return noise_pred_fn(x, t_continuous) |
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elif guidance_type == "classifier": |
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assert classifier_fn is not None |
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t_input = get_model_input_time(t_continuous) |
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cond_grad = cond_grad_fn(x, t_input) |
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sigma_t = noise_schedule.marginal_std(t_continuous) |
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noise = noise_pred_fn(x, t_continuous) |
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return noise - guidance_scale * expand_dims(sigma_t, dims=cond_grad.dim()) * cond_grad |
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elif guidance_type == "classifier-free": |
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if guidance_scale == 1. or unconditional_condition is None: |
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return noise_pred_fn(x, t_continuous, cond=condition) |
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else: |
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x_in = torch.cat([x] * 2) |
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t_in = torch.cat([t_continuous] * 2) |
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if isinstance(condition, dict): |
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assert isinstance(unconditional_condition, dict) |
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c_in = dict() |
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for k in condition: |
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if isinstance(condition[k], list): |
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c_in[k] = [torch.cat([unconditional_condition[k][i], condition[k][i]]) for i in range(len(condition[k]))] |
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else: |
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c_in[k] = torch.cat([unconditional_condition[k], condition[k]]) |
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else: |
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c_in = torch.cat([unconditional_condition, condition]) |
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noise_uncond, noise = noise_pred_fn(x_in, t_in, cond=c_in).chunk(2) |
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return noise_uncond + guidance_scale * (noise - noise_uncond) |
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|
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assert model_type in ["noise", "x_start", "v"] |
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assert guidance_type in ["uncond", "classifier", "classifier-free"] |
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return model_fn |
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|
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class DPM_Solver: |
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def __init__(self, model_fn, noise_schedule, predict_x0=False, thresholding=False, max_val=1.): |
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"""Construct a DPM-Solver. |
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We support both the noise prediction model ("predicting epsilon") and the data prediction model ("predicting x0"). |
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If `predict_x0` is False, we use the solver for the noise prediction model (DPM-Solver). |
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If `predict_x0` is True, we use the solver for the data prediction model (DPM-Solver++). |
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In such case, we further support the "dynamic thresholding" in [1] when `thresholding` is True. |
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The "dynamic thresholding" can greatly improve the sample quality for pixel-space DPMs with large guidance scales. |
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Args: |
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model_fn: A noise prediction model function which accepts the continuous-time input (t in [epsilon, T]): |
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`` |
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def model_fn(x, t_continuous): |
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return noise |
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`` |
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noise_schedule: A noise schedule object, such as NoiseScheduleVP. |
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predict_x0: A `bool`. If true, use the data prediction model; else, use the noise prediction model. |
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thresholding: A `bool`. Valid when `predict_x0` is True. Whether to use the "dynamic thresholding" in [1]. |
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max_val: A `float`. Valid when both `predict_x0` and `thresholding` are True. The max value for thresholding. |
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|
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[1] Chitwan Saharia, William Chan, Saurabh Saxena, Lala Li, Jay Whang, Emily Denton, Seyed Kamyar Seyed Ghasemipour, Burcu Karagol Ayan, S Sara Mahdavi, Rapha Gontijo Lopes, et al. Photorealistic text-to-image diffusion models with deep language understanding. arXiv preprint arXiv:2205.11487, 2022b. |
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""" |
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self.model = model_fn |
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self.noise_schedule = noise_schedule |
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self.predict_x0 = predict_x0 |
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self.thresholding = thresholding |
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self.max_val = max_val |
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|
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def noise_prediction_fn(self, x, t): |
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""" |
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Return the noise prediction model. |
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""" |
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return self.model(x, t) |
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|
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def data_prediction_fn(self, x, t): |
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""" |
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Return the data prediction model (with thresholding). |
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""" |
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noise = self.noise_prediction_fn(x, t) |
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dims = x.dim() |
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alpha_t, sigma_t = self.noise_schedule.marginal_alpha(t), self.noise_schedule.marginal_std(t) |
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x0 = (x - expand_dims(sigma_t, dims) * noise) / expand_dims(alpha_t, dims) |
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if self.thresholding: |
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p = 0.995 |
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s = torch.quantile(torch.abs(x0).reshape((x0.shape[0], -1)), p, dim=1) |
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s = expand_dims(torch.maximum(s, self.max_val * torch.ones_like(s).to(s.device)), dims) |
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x0 = torch.clamp(x0, -s, s) / s |
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return x0 |
|
|
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def model_fn(self, x, t): |
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""" |
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Convert the model to the noise prediction model or the data prediction model. |
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""" |
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if self.predict_x0: |
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return self.data_prediction_fn(x, t) |
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else: |
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return self.noise_prediction_fn(x, t) |
|
|
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def get_time_steps(self, skip_type, t_T, t_0, N, device): |
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"""Compute the intermediate time steps for sampling. |
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Args: |
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skip_type: A `str`. The type for the spacing of the time steps. We support three types: |
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- 'logSNR': uniform logSNR for the time steps. |
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- 'time_uniform': uniform time for the time steps. (**Recommended for high-resolutional data**.) |
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- 'time_quadratic': quadratic time for the time steps. (Used in DDIM for low-resolutional data.) |
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t_T: A `float`. The starting time of the sampling (default is T). |
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t_0: A `float`. The ending time of the sampling (default is epsilon). |
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N: A `int`. The total number of the spacing of the time steps. |
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device: A torch device. |
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Returns: |
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A pytorch tensor of the time steps, with the shape (N + 1,). |
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""" |
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if skip_type == 'logSNR': |
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lambda_T = self.noise_schedule.marginal_lambda(torch.tensor(t_T).to(device)) |
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lambda_0 = self.noise_schedule.marginal_lambda(torch.tensor(t_0).to(device)) |
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logSNR_steps = torch.linspace(lambda_T.cpu().item(), lambda_0.cpu().item(), N + 1).to(device) |
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return self.noise_schedule.inverse_lambda(logSNR_steps) |
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elif skip_type == 'time_uniform': |
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return torch.linspace(t_T, t_0, N + 1).to(device) |
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elif skip_type == 'time_quadratic': |
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t_order = 2 |
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t = torch.linspace(t_T ** (1. / t_order), t_0 ** (1. / t_order), N + 1).pow(t_order).to(device) |
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return t |
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else: |
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raise ValueError( |
|
"Unsupported skip_type {}, need to be 'logSNR' or 'time_uniform' or 'time_quadratic'".format(skip_type)) |
|
|
|
def get_orders_and_timesteps_for_singlestep_solver(self, steps, order, skip_type, t_T, t_0, device): |
|
""" |
|
Get the order of each step for sampling by the singlestep DPM-Solver. |
|
We combine both DPM-Solver-1,2,3 to use all the function evaluations, which is named as "DPM-Solver-fast". |
|
Given a fixed number of function evaluations by `steps`, the sampling procedure by DPM-Solver-fast is: |
|
- If order == 1: |
|
We take `steps` of DPM-Solver-1 (i.e. DDIM). |
|
- If order == 2: |
|
- Denote K = (steps // 2). We take K or (K + 1) intermediate time steps for sampling. |
|
- If steps % 2 == 0, we use K steps of DPM-Solver-2. |
|
- If steps % 2 == 1, we use K steps of DPM-Solver-2 and 1 step of DPM-Solver-1. |
|
- If order == 3: |
|
- Denote K = (steps // 3 + 1). We take K intermediate time steps for sampling. |
|
- If steps % 3 == 0, we use (K - 2) steps of DPM-Solver-3, and 1 step of DPM-Solver-2 and 1 step of DPM-Solver-1. |
|
- If steps % 3 == 1, we use (K - 1) steps of DPM-Solver-3 and 1 step of DPM-Solver-1. |
|
- If steps % 3 == 2, we use (K - 1) steps of DPM-Solver-3 and 1 step of DPM-Solver-2. |
|
============================================ |
|
Args: |
|
order: A `int`. The max order for the solver (2 or 3). |
|
steps: A `int`. The total number of function evaluations (NFE). |
|
skip_type: A `str`. The type for the spacing of the time steps. We support three types: |
|
- 'logSNR': uniform logSNR for the time steps. |
|
- 'time_uniform': uniform time for the time steps. (**Recommended for high-resolutional data**.) |
|
- 'time_quadratic': quadratic time for the time steps. (Used in DDIM for low-resolutional data.) |
|
t_T: A `float`. The starting time of the sampling (default is T). |
|
t_0: A `float`. The ending time of the sampling (default is epsilon). |
|
device: A torch device. |
|
Returns: |
|
orders: A list of the solver order of each step. |
|
""" |
|
if order == 3: |
|
K = steps // 3 + 1 |
|
if steps % 3 == 0: |
|
orders = [3, ] * (K - 2) + [2, 1] |
|
elif steps % 3 == 1: |
|
orders = [3, ] * (K - 1) + [1] |
|
else: |
|
orders = [3, ] * (K - 1) + [2] |
|
elif order == 2: |
|
if steps % 2 == 0: |
|
K = steps // 2 |
|
orders = [2, ] * K |
|
else: |
|
K = steps // 2 + 1 |
|
orders = [2, ] * (K - 1) + [1] |
|
elif order == 1: |
|
K = 1 |
|
orders = [1, ] * steps |
|
else: |
|
raise ValueError("'order' must be '1' or '2' or '3'.") |
|
if skip_type == 'logSNR': |
|
|
|
timesteps_outer = self.get_time_steps(skip_type, t_T, t_0, K, device) |
|
else: |
|
timesteps_outer = self.get_time_steps(skip_type, t_T, t_0, steps, device)[ |
|
torch.cumsum(torch.tensor([0, ] + orders)).to(device)] |
|
return timesteps_outer, orders |
|
|
|
def denoise_to_zero_fn(self, x, s): |
|
""" |
|
Denoise at the final step, which is equivalent to solve the ODE from lambda_s to infty by first-order discretization. |
|
""" |
|
return self.data_prediction_fn(x, s) |
|
|
|
def dpm_solver_first_update(self, x, s, t, model_s=None, return_intermediate=False): |
|
""" |
|
DPM-Solver-1 (equivalent to DDIM) from time `s` to time `t`. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `s`. |
|
s: A pytorch tensor. The starting time, with the shape (x.shape[0],). |
|
t: A pytorch tensor. The ending time, with the shape (x.shape[0],). |
|
model_s: A pytorch tensor. The model function evaluated at time `s`. |
|
If `model_s` is None, we evaluate the model by `x` and `s`; otherwise we directly use it. |
|
return_intermediate: A `bool`. If true, also return the model value at time `s`. |
|
Returns: |
|
x_t: A pytorch tensor. The approximated solution at time `t`. |
|
""" |
|
ns = self.noise_schedule |
|
dims = x.dim() |
|
lambda_s, lambda_t = ns.marginal_lambda(s), ns.marginal_lambda(t) |
|
h = lambda_t - lambda_s |
|
log_alpha_s, log_alpha_t = ns.marginal_log_mean_coeff(s), ns.marginal_log_mean_coeff(t) |
|
sigma_s, sigma_t = ns.marginal_std(s), ns.marginal_std(t) |
|
alpha_t = torch.exp(log_alpha_t) |
|
|
|
if self.predict_x0: |
|
phi_1 = torch.expm1(-h) |
|
if model_s is None: |
|
model_s = self.model_fn(x, s) |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_s, dims) * x |
|
- expand_dims(alpha_t * phi_1, dims) * model_s |
|
) |
|
if return_intermediate: |
|
return x_t, {'model_s': model_s} |
|
else: |
|
return x_t |
|
else: |
|
phi_1 = torch.expm1(h) |
|
if model_s is None: |
|
model_s = self.model_fn(x, s) |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_s), dims) * x |
|
- expand_dims(sigma_t * phi_1, dims) * model_s |
|
) |
|
if return_intermediate: |
|
return x_t, {'model_s': model_s} |
|
else: |
|
return x_t |
|
|
|
def singlestep_dpm_solver_second_update(self, x, s, t, r1=0.5, model_s=None, return_intermediate=False, |
|
solver_type='dpm_solver'): |
|
""" |
|
Singlestep solver DPM-Solver-2 from time `s` to time `t`. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `s`. |
|
s: A pytorch tensor. The starting time, with the shape (x.shape[0],). |
|
t: A pytorch tensor. The ending time, with the shape (x.shape[0],). |
|
r1: A `float`. The hyperparameter of the second-order solver. |
|
model_s: A pytorch tensor. The model function evaluated at time `s`. |
|
If `model_s` is None, we evaluate the model by `x` and `s`; otherwise we directly use it. |
|
return_intermediate: A `bool`. If true, also return the model value at time `s` and `s1` (the intermediate time). |
|
solver_type: either 'dpm_solver' or 'taylor'. The type for the high-order solvers. |
|
The type slightly impacts the performance. We recommend to use 'dpm_solver' type. |
|
Returns: |
|
x_t: A pytorch tensor. The approximated solution at time `t`. |
|
""" |
|
if solver_type not in ['dpm_solver', 'taylor']: |
|
raise ValueError("'solver_type' must be either 'dpm_solver' or 'taylor', got {}".format(solver_type)) |
|
if r1 is None: |
|
r1 = 0.5 |
|
ns = self.noise_schedule |
|
dims = x.dim() |
|
lambda_s, lambda_t = ns.marginal_lambda(s), ns.marginal_lambda(t) |
|
h = lambda_t - lambda_s |
|
lambda_s1 = lambda_s + r1 * h |
|
s1 = ns.inverse_lambda(lambda_s1) |
|
log_alpha_s, log_alpha_s1, log_alpha_t = ns.marginal_log_mean_coeff(s), ns.marginal_log_mean_coeff( |
|
s1), ns.marginal_log_mean_coeff(t) |
|
sigma_s, sigma_s1, sigma_t = ns.marginal_std(s), ns.marginal_std(s1), ns.marginal_std(t) |
|
alpha_s1, alpha_t = torch.exp(log_alpha_s1), torch.exp(log_alpha_t) |
|
|
|
if self.predict_x0: |
|
phi_11 = torch.expm1(-r1 * h) |
|
phi_1 = torch.expm1(-h) |
|
|
|
if model_s is None: |
|
model_s = self.model_fn(x, s) |
|
x_s1 = ( |
|
expand_dims(sigma_s1 / sigma_s, dims) * x |
|
- expand_dims(alpha_s1 * phi_11, dims) * model_s |
|
) |
|
model_s1 = self.model_fn(x_s1, s1) |
|
if solver_type == 'dpm_solver': |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_s, dims) * x |
|
- expand_dims(alpha_t * phi_1, dims) * model_s |
|
- (0.5 / r1) * expand_dims(alpha_t * phi_1, dims) * (model_s1 - model_s) |
|
) |
|
elif solver_type == 'taylor': |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_s, dims) * x |
|
- expand_dims(alpha_t * phi_1, dims) * model_s |
|
+ (1. / r1) * expand_dims(alpha_t * ((torch.exp(-h) - 1.) / h + 1.), dims) * ( |
|
model_s1 - model_s) |
|
) |
|
else: |
|
phi_11 = torch.expm1(r1 * h) |
|
phi_1 = torch.expm1(h) |
|
|
|
if model_s is None: |
|
model_s = self.model_fn(x, s) |
|
x_s1 = ( |
|
expand_dims(torch.exp(log_alpha_s1 - log_alpha_s), dims) * x |
|
- expand_dims(sigma_s1 * phi_11, dims) * model_s |
|
) |
|
model_s1 = self.model_fn(x_s1, s1) |
|
if solver_type == 'dpm_solver': |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_s), dims) * x |
|
- expand_dims(sigma_t * phi_1, dims) * model_s |
|
- (0.5 / r1) * expand_dims(sigma_t * phi_1, dims) * (model_s1 - model_s) |
|
) |
|
elif solver_type == 'taylor': |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_s), dims) * x |
|
- expand_dims(sigma_t * phi_1, dims) * model_s |
|
- (1. / r1) * expand_dims(sigma_t * ((torch.exp(h) - 1.) / h - 1.), dims) * (model_s1 - model_s) |
|
) |
|
if return_intermediate: |
|
return x_t, {'model_s': model_s, 'model_s1': model_s1} |
|
else: |
|
return x_t |
|
|
|
def singlestep_dpm_solver_third_update(self, x, s, t, r1=1. / 3., r2=2. / 3., model_s=None, model_s1=None, |
|
return_intermediate=False, solver_type='dpm_solver'): |
|
""" |
|
Singlestep solver DPM-Solver-3 from time `s` to time `t`. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `s`. |
|
s: A pytorch tensor. The starting time, with the shape (x.shape[0],). |
|
t: A pytorch tensor. The ending time, with the shape (x.shape[0],). |
|
r1: A `float`. The hyperparameter of the third-order solver. |
|
r2: A `float`. The hyperparameter of the third-order solver. |
|
model_s: A pytorch tensor. The model function evaluated at time `s`. |
|
If `model_s` is None, we evaluate the model by `x` and `s`; otherwise we directly use it. |
|
model_s1: A pytorch tensor. The model function evaluated at time `s1` (the intermediate time given by `r1`). |
|
If `model_s1` is None, we evaluate the model at `s1`; otherwise we directly use it. |
|
return_intermediate: A `bool`. If true, also return the model value at time `s`, `s1` and `s2` (the intermediate times). |
|
solver_type: either 'dpm_solver' or 'taylor'. The type for the high-order solvers. |
|
The type slightly impacts the performance. We recommend to use 'dpm_solver' type. |
|
Returns: |
|
x_t: A pytorch tensor. The approximated solution at time `t`. |
|
""" |
|
if solver_type not in ['dpm_solver', 'taylor']: |
|
raise ValueError("'solver_type' must be either 'dpm_solver' or 'taylor', got {}".format(solver_type)) |
|
if r1 is None: |
|
r1 = 1. / 3. |
|
if r2 is None: |
|
r2 = 2. / 3. |
|
ns = self.noise_schedule |
|
dims = x.dim() |
|
lambda_s, lambda_t = ns.marginal_lambda(s), ns.marginal_lambda(t) |
|
h = lambda_t - lambda_s |
|
lambda_s1 = lambda_s + r1 * h |
|
lambda_s2 = lambda_s + r2 * h |
|
s1 = ns.inverse_lambda(lambda_s1) |
|
s2 = ns.inverse_lambda(lambda_s2) |
|
log_alpha_s, log_alpha_s1, log_alpha_s2, log_alpha_t = ns.marginal_log_mean_coeff( |
|
s), ns.marginal_log_mean_coeff(s1), ns.marginal_log_mean_coeff(s2), ns.marginal_log_mean_coeff(t) |
|
sigma_s, sigma_s1, sigma_s2, sigma_t = ns.marginal_std(s), ns.marginal_std(s1), ns.marginal_std( |
|
s2), ns.marginal_std(t) |
|
alpha_s1, alpha_s2, alpha_t = torch.exp(log_alpha_s1), torch.exp(log_alpha_s2), torch.exp(log_alpha_t) |
|
|
|
if self.predict_x0: |
|
phi_11 = torch.expm1(-r1 * h) |
|
phi_12 = torch.expm1(-r2 * h) |
|
phi_1 = torch.expm1(-h) |
|
phi_22 = torch.expm1(-r2 * h) / (r2 * h) + 1. |
|
phi_2 = phi_1 / h + 1. |
|
phi_3 = phi_2 / h - 0.5 |
|
|
|
if model_s is None: |
|
model_s = self.model_fn(x, s) |
|
if model_s1 is None: |
|
x_s1 = ( |
|
expand_dims(sigma_s1 / sigma_s, dims) * x |
|
- expand_dims(alpha_s1 * phi_11, dims) * model_s |
|
) |
|
model_s1 = self.model_fn(x_s1, s1) |
|
x_s2 = ( |
|
expand_dims(sigma_s2 / sigma_s, dims) * x |
|
- expand_dims(alpha_s2 * phi_12, dims) * model_s |
|
+ r2 / r1 * expand_dims(alpha_s2 * phi_22, dims) * (model_s1 - model_s) |
|
) |
|
model_s2 = self.model_fn(x_s2, s2) |
|
if solver_type == 'dpm_solver': |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_s, dims) * x |
|
- expand_dims(alpha_t * phi_1, dims) * model_s |
|
+ (1. / r2) * expand_dims(alpha_t * phi_2, dims) * (model_s2 - model_s) |
|
) |
|
elif solver_type == 'taylor': |
|
D1_0 = (1. / r1) * (model_s1 - model_s) |
|
D1_1 = (1. / r2) * (model_s2 - model_s) |
|
D1 = (r2 * D1_0 - r1 * D1_1) / (r2 - r1) |
|
D2 = 2. * (D1_1 - D1_0) / (r2 - r1) |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_s, dims) * x |
|
- expand_dims(alpha_t * phi_1, dims) * model_s |
|
+ expand_dims(alpha_t * phi_2, dims) * D1 |
|
- expand_dims(alpha_t * phi_3, dims) * D2 |
|
) |
|
else: |
|
phi_11 = torch.expm1(r1 * h) |
|
phi_12 = torch.expm1(r2 * h) |
|
phi_1 = torch.expm1(h) |
|
phi_22 = torch.expm1(r2 * h) / (r2 * h) - 1. |
|
phi_2 = phi_1 / h - 1. |
|
phi_3 = phi_2 / h - 0.5 |
|
|
|
if model_s is None: |
|
model_s = self.model_fn(x, s) |
|
if model_s1 is None: |
|
x_s1 = ( |
|
expand_dims(torch.exp(log_alpha_s1 - log_alpha_s), dims) * x |
|
- expand_dims(sigma_s1 * phi_11, dims) * model_s |
|
) |
|
model_s1 = self.model_fn(x_s1, s1) |
|
x_s2 = ( |
|
expand_dims(torch.exp(log_alpha_s2 - log_alpha_s), dims) * x |
|
- expand_dims(sigma_s2 * phi_12, dims) * model_s |
|
- r2 / r1 * expand_dims(sigma_s2 * phi_22, dims) * (model_s1 - model_s) |
|
) |
|
model_s2 = self.model_fn(x_s2, s2) |
|
if solver_type == 'dpm_solver': |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_s), dims) * x |
|
- expand_dims(sigma_t * phi_1, dims) * model_s |
|
- (1. / r2) * expand_dims(sigma_t * phi_2, dims) * (model_s2 - model_s) |
|
) |
|
elif solver_type == 'taylor': |
|
D1_0 = (1. / r1) * (model_s1 - model_s) |
|
D1_1 = (1. / r2) * (model_s2 - model_s) |
|
D1 = (r2 * D1_0 - r1 * D1_1) / (r2 - r1) |
|
D2 = 2. * (D1_1 - D1_0) / (r2 - r1) |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_s), dims) * x |
|
- expand_dims(sigma_t * phi_1, dims) * model_s |
|
- expand_dims(sigma_t * phi_2, dims) * D1 |
|
- expand_dims(sigma_t * phi_3, dims) * D2 |
|
) |
|
|
|
if return_intermediate: |
|
return x_t, {'model_s': model_s, 'model_s1': model_s1, 'model_s2': model_s2} |
|
else: |
|
return x_t |
|
|
|
def multistep_dpm_solver_second_update(self, x, model_prev_list, t_prev_list, t, solver_type="dpm_solver"): |
|
""" |
|
Multistep solver DPM-Solver-2 from time `t_prev_list[-1]` to time `t`. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `s`. |
|
model_prev_list: A list of pytorch tensor. The previous computed model values. |
|
t_prev_list: A list of pytorch tensor. The previous times, each time has the shape (x.shape[0],) |
|
t: A pytorch tensor. The ending time, with the shape (x.shape[0],). |
|
solver_type: either 'dpm_solver' or 'taylor'. The type for the high-order solvers. |
|
The type slightly impacts the performance. We recommend to use 'dpm_solver' type. |
|
Returns: |
|
x_t: A pytorch tensor. The approximated solution at time `t`. |
|
""" |
|
if solver_type not in ['dpm_solver', 'taylor']: |
|
raise ValueError("'solver_type' must be either 'dpm_solver' or 'taylor', got {}".format(solver_type)) |
|
ns = self.noise_schedule |
|
dims = x.dim() |
|
model_prev_1, model_prev_0 = model_prev_list |
|
t_prev_1, t_prev_0 = t_prev_list |
|
lambda_prev_1, lambda_prev_0, lambda_t = ns.marginal_lambda(t_prev_1), ns.marginal_lambda( |
|
t_prev_0), ns.marginal_lambda(t) |
|
log_alpha_prev_0, log_alpha_t = ns.marginal_log_mean_coeff(t_prev_0), ns.marginal_log_mean_coeff(t) |
|
sigma_prev_0, sigma_t = ns.marginal_std(t_prev_0), ns.marginal_std(t) |
|
alpha_t = torch.exp(log_alpha_t) |
|
|
|
h_0 = lambda_prev_0 - lambda_prev_1 |
|
h = lambda_t - lambda_prev_0 |
|
r0 = h_0 / h |
|
D1_0 = expand_dims(1. / r0, dims) * (model_prev_0 - model_prev_1) |
|
if self.predict_x0: |
|
if solver_type == 'dpm_solver': |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_prev_0, dims) * x |
|
- expand_dims(alpha_t * (torch.exp(-h) - 1.), dims) * model_prev_0 |
|
- 0.5 * expand_dims(alpha_t * (torch.exp(-h) - 1.), dims) * D1_0 |
|
) |
|
elif solver_type == 'taylor': |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_prev_0, dims) * x |
|
- expand_dims(alpha_t * (torch.exp(-h) - 1.), dims) * model_prev_0 |
|
+ expand_dims(alpha_t * ((torch.exp(-h) - 1.) / h + 1.), dims) * D1_0 |
|
) |
|
else: |
|
if solver_type == 'dpm_solver': |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_prev_0), dims) * x |
|
- expand_dims(sigma_t * (torch.exp(h) - 1.), dims) * model_prev_0 |
|
- 0.5 * expand_dims(sigma_t * (torch.exp(h) - 1.), dims) * D1_0 |
|
) |
|
elif solver_type == 'taylor': |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_prev_0), dims) * x |
|
- expand_dims(sigma_t * (torch.exp(h) - 1.), dims) * model_prev_0 |
|
- expand_dims(sigma_t * ((torch.exp(h) - 1.) / h - 1.), dims) * D1_0 |
|
) |
|
return x_t |
|
|
|
def multistep_dpm_solver_third_update(self, x, model_prev_list, t_prev_list, t, solver_type='dpm_solver'): |
|
""" |
|
Multistep solver DPM-Solver-3 from time `t_prev_list[-1]` to time `t`. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `s`. |
|
model_prev_list: A list of pytorch tensor. The previous computed model values. |
|
t_prev_list: A list of pytorch tensor. The previous times, each time has the shape (x.shape[0],) |
|
t: A pytorch tensor. The ending time, with the shape (x.shape[0],). |
|
solver_type: either 'dpm_solver' or 'taylor'. The type for the high-order solvers. |
|
The type slightly impacts the performance. We recommend to use 'dpm_solver' type. |
|
Returns: |
|
x_t: A pytorch tensor. The approximated solution at time `t`. |
|
""" |
|
ns = self.noise_schedule |
|
dims = x.dim() |
|
model_prev_2, model_prev_1, model_prev_0 = model_prev_list |
|
t_prev_2, t_prev_1, t_prev_0 = t_prev_list |
|
lambda_prev_2, lambda_prev_1, lambda_prev_0, lambda_t = ns.marginal_lambda(t_prev_2), ns.marginal_lambda( |
|
t_prev_1), ns.marginal_lambda(t_prev_0), ns.marginal_lambda(t) |
|
log_alpha_prev_0, log_alpha_t = ns.marginal_log_mean_coeff(t_prev_0), ns.marginal_log_mean_coeff(t) |
|
sigma_prev_0, sigma_t = ns.marginal_std(t_prev_0), ns.marginal_std(t) |
|
alpha_t = torch.exp(log_alpha_t) |
|
|
|
h_1 = lambda_prev_1 - lambda_prev_2 |
|
h_0 = lambda_prev_0 - lambda_prev_1 |
|
h = lambda_t - lambda_prev_0 |
|
r0, r1 = h_0 / h, h_1 / h |
|
D1_0 = expand_dims(1. / r0, dims) * (model_prev_0 - model_prev_1) |
|
D1_1 = expand_dims(1. / r1, dims) * (model_prev_1 - model_prev_2) |
|
D1 = D1_0 + expand_dims(r0 / (r0 + r1), dims) * (D1_0 - D1_1) |
|
D2 = expand_dims(1. / (r0 + r1), dims) * (D1_0 - D1_1) |
|
if self.predict_x0: |
|
x_t = ( |
|
expand_dims(sigma_t / sigma_prev_0, dims) * x |
|
- expand_dims(alpha_t * (torch.exp(-h) - 1.), dims) * model_prev_0 |
|
+ expand_dims(alpha_t * ((torch.exp(-h) - 1.) / h + 1.), dims) * D1 |
|
- expand_dims(alpha_t * ((torch.exp(-h) - 1. + h) / h ** 2 - 0.5), dims) * D2 |
|
) |
|
else: |
|
x_t = ( |
|
expand_dims(torch.exp(log_alpha_t - log_alpha_prev_0), dims) * x |
|
- expand_dims(sigma_t * (torch.exp(h) - 1.), dims) * model_prev_0 |
|
- expand_dims(sigma_t * ((torch.exp(h) - 1.) / h - 1.), dims) * D1 |
|
- expand_dims(sigma_t * ((torch.exp(h) - 1. - h) / h ** 2 - 0.5), dims) * D2 |
|
) |
|
return x_t |
|
|
|
def singlestep_dpm_solver_update(self, x, s, t, order, return_intermediate=False, solver_type='dpm_solver', r1=None, |
|
r2=None): |
|
""" |
|
Singlestep DPM-Solver with the order `order` from time `s` to time `t`. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `s`. |
|
s: A pytorch tensor. The starting time, with the shape (x.shape[0],). |
|
t: A pytorch tensor. The ending time, with the shape (x.shape[0],). |
|
order: A `int`. The order of DPM-Solver. We only support order == 1 or 2 or 3. |
|
return_intermediate: A `bool`. If true, also return the model value at time `s`, `s1` and `s2` (the intermediate times). |
|
solver_type: either 'dpm_solver' or 'taylor'. The type for the high-order solvers. |
|
The type slightly impacts the performance. We recommend to use 'dpm_solver' type. |
|
r1: A `float`. The hyperparameter of the second-order or third-order solver. |
|
r2: A `float`. The hyperparameter of the third-order solver. |
|
Returns: |
|
x_t: A pytorch tensor. The approximated solution at time `t`. |
|
""" |
|
if order == 1: |
|
return self.dpm_solver_first_update(x, s, t, return_intermediate=return_intermediate) |
|
elif order == 2: |
|
return self.singlestep_dpm_solver_second_update(x, s, t, return_intermediate=return_intermediate, |
|
solver_type=solver_type, r1=r1) |
|
elif order == 3: |
|
return self.singlestep_dpm_solver_third_update(x, s, t, return_intermediate=return_intermediate, |
|
solver_type=solver_type, r1=r1, r2=r2) |
|
else: |
|
raise ValueError("Solver order must be 1 or 2 or 3, got {}".format(order)) |
|
|
|
def multistep_dpm_solver_update(self, x, model_prev_list, t_prev_list, t, order, solver_type='dpm_solver'): |
|
""" |
|
Multistep DPM-Solver with the order `order` from time `t_prev_list[-1]` to time `t`. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `s`. |
|
model_prev_list: A list of pytorch tensor. The previous computed model values. |
|
t_prev_list: A list of pytorch tensor. The previous times, each time has the shape (x.shape[0],) |
|
t: A pytorch tensor. The ending time, with the shape (x.shape[0],). |
|
order: A `int`. The order of DPM-Solver. We only support order == 1 or 2 or 3. |
|
solver_type: either 'dpm_solver' or 'taylor'. The type for the high-order solvers. |
|
The type slightly impacts the performance. We recommend to use 'dpm_solver' type. |
|
Returns: |
|
x_t: A pytorch tensor. The approximated solution at time `t`. |
|
""" |
|
if order == 1: |
|
return self.dpm_solver_first_update(x, t_prev_list[-1], t, model_s=model_prev_list[-1]) |
|
elif order == 2: |
|
return self.multistep_dpm_solver_second_update(x, model_prev_list, t_prev_list, t, solver_type=solver_type) |
|
elif order == 3: |
|
return self.multistep_dpm_solver_third_update(x, model_prev_list, t_prev_list, t, solver_type=solver_type) |
|
else: |
|
raise ValueError("Solver order must be 1 or 2 or 3, got {}".format(order)) |
|
|
|
def dpm_solver_adaptive(self, x, order, t_T, t_0, h_init=0.05, atol=0.0078, rtol=0.05, theta=0.9, t_err=1e-5, |
|
solver_type='dpm_solver'): |
|
""" |
|
The adaptive step size solver based on singlestep DPM-Solver. |
|
Args: |
|
x: A pytorch tensor. The initial value at time `t_T`. |
|
order: A `int`. The (higher) order of the solver. We only support order == 2 or 3. |
|
t_T: A `float`. The starting time of the sampling (default is T). |
|
t_0: A `float`. The ending time of the sampling (default is epsilon). |
|
h_init: A `float`. The initial step size (for logSNR). |
|
atol: A `float`. The absolute tolerance of the solver. For image data, the default setting is 0.0078, followed [1]. |
|
rtol: A `float`. The relative tolerance of the solver. The default setting is 0.05. |
|
theta: A `float`. The safety hyperparameter for adapting the step size. The default setting is 0.9, followed [1]. |
|
t_err: A `float`. The tolerance for the time. We solve the diffusion ODE until the absolute error between the |
|
current time and `t_0` is less than `t_err`. The default setting is 1e-5. |
|
solver_type: either 'dpm_solver' or 'taylor'. The type for the high-order solvers. |
|
The type slightly impacts the performance. We recommend to use 'dpm_solver' type. |
|
Returns: |
|
x_0: A pytorch tensor. The approximated solution at time `t_0`. |
|
[1] A. Jolicoeur-Martineau, K. Li, R. Piché-Taillefer, T. Kachman, and I. Mitliagkas, "Gotta go fast when generating data with score-based models," arXiv preprint arXiv:2105.14080, 2021. |
|
""" |
|
ns = self.noise_schedule |
|
s = t_T * torch.ones((x.shape[0],)).to(x) |
|
lambda_s = ns.marginal_lambda(s) |
|
lambda_0 = ns.marginal_lambda(t_0 * torch.ones_like(s).to(x)) |
|
h = h_init * torch.ones_like(s).to(x) |
|
x_prev = x |
|
nfe = 0 |
|
if order == 2: |
|
r1 = 0.5 |
|
lower_update = lambda x, s, t: self.dpm_solver_first_update(x, s, t, return_intermediate=True) |
|
higher_update = lambda x, s, t, **kwargs: self.singlestep_dpm_solver_second_update(x, s, t, r1=r1, |
|
solver_type=solver_type, |
|
**kwargs) |
|
elif order == 3: |
|
r1, r2 = 1. / 3., 2. / 3. |
|
lower_update = lambda x, s, t: self.singlestep_dpm_solver_second_update(x, s, t, r1=r1, |
|
return_intermediate=True, |
|
solver_type=solver_type) |
|
higher_update = lambda x, s, t, **kwargs: self.singlestep_dpm_solver_third_update(x, s, t, r1=r1, r2=r2, |
|
solver_type=solver_type, |
|
**kwargs) |
|
else: |
|
raise ValueError("For adaptive step size solver, order must be 2 or 3, got {}".format(order)) |
|
while torch.abs((s - t_0)).mean() > t_err: |
|
t = ns.inverse_lambda(lambda_s + h) |
|
x_lower, lower_noise_kwargs = lower_update(x, s, t) |
|
x_higher = higher_update(x, s, t, **lower_noise_kwargs) |
|
delta = torch.max(torch.ones_like(x).to(x) * atol, rtol * torch.max(torch.abs(x_lower), torch.abs(x_prev))) |
|
norm_fn = lambda v: torch.sqrt(torch.square(v.reshape((v.shape[0], -1))).mean(dim=-1, keepdim=True)) |
|
E = norm_fn((x_higher - x_lower) / delta).max() |
|
if torch.all(E <= 1.): |
|
x = x_higher |
|
s = t |
|
x_prev = x_lower |
|
lambda_s = ns.marginal_lambda(s) |
|
h = torch.min(theta * h * torch.float_power(E, -1. / order).float(), lambda_0 - lambda_s) |
|
nfe += order |
|
print('adaptive solver nfe', nfe) |
|
return x |
|
|
|
def sample(self, x, steps=20, t_start=None, t_end=None, order=3, skip_type='time_uniform', |
|
method='singlestep', lower_order_final=True, denoise_to_zero=False, solver_type='dpm_solver', |
|
atol=0.0078, rtol=0.05, |
|
): |
|
""" |
|
Compute the sample at time `t_end` by DPM-Solver, given the initial `x` at time `t_start`. |
|
===================================================== |
|
We support the following algorithms for both noise prediction model and data prediction model: |
|
- 'singlestep': |
|
Singlestep DPM-Solver (i.e. "DPM-Solver-fast" in the paper), which combines different orders of singlestep DPM-Solver. |
|
We combine all the singlestep solvers with order <= `order` to use up all the function evaluations (steps). |
|
The total number of function evaluations (NFE) == `steps`. |
|
Given a fixed NFE == `steps`, the sampling procedure is: |
|
- If `order` == 1: |
|
- Denote K = steps. We use K steps of DPM-Solver-1 (i.e. DDIM). |
|
- If `order` == 2: |
|
- Denote K = (steps // 2) + (steps % 2). We take K intermediate time steps for sampling. |
|
- If steps % 2 == 0, we use K steps of singlestep DPM-Solver-2. |
|
- If steps % 2 == 1, we use (K - 1) steps of singlestep DPM-Solver-2 and 1 step of DPM-Solver-1. |
|
- If `order` == 3: |
|
- Denote K = (steps // 3 + 1). We take K intermediate time steps for sampling. |
|
- If steps % 3 == 0, we use (K - 2) steps of singlestep DPM-Solver-3, and 1 step of singlestep DPM-Solver-2 and 1 step of DPM-Solver-1. |
|
- If steps % 3 == 1, we use (K - 1) steps of singlestep DPM-Solver-3 and 1 step of DPM-Solver-1. |
|
- If steps % 3 == 2, we use (K - 1) steps of singlestep DPM-Solver-3 and 1 step of singlestep DPM-Solver-2. |
|
- 'multistep': |
|
Multistep DPM-Solver with the order of `order`. The total number of function evaluations (NFE) == `steps`. |
|
We initialize the first `order` values by lower order multistep solvers. |
|
Given a fixed NFE == `steps`, the sampling procedure is: |
|
Denote K = steps. |
|
- If `order` == 1: |
|
- We use K steps of DPM-Solver-1 (i.e. DDIM). |
|
- If `order` == 2: |
|
- We firstly use 1 step of DPM-Solver-1, then use (K - 1) step of multistep DPM-Solver-2. |
|
- If `order` == 3: |
|
- We firstly use 1 step of DPM-Solver-1, then 1 step of multistep DPM-Solver-2, then (K - 2) step of multistep DPM-Solver-3. |
|
- 'singlestep_fixed': |
|
Fixed order singlestep DPM-Solver (i.e. DPM-Solver-1 or singlestep DPM-Solver-2 or singlestep DPM-Solver-3). |
|
We use singlestep DPM-Solver-`order` for `order`=1 or 2 or 3, with total [`steps` // `order`] * `order` NFE. |
|
- 'adaptive': |
|
Adaptive step size DPM-Solver (i.e. "DPM-Solver-12" and "DPM-Solver-23" in the paper). |
|
We ignore `steps` and use adaptive step size DPM-Solver with a higher order of `order`. |
|
You can adjust the absolute tolerance `atol` and the relative tolerance `rtol` to balance the computatation costs |
|
(NFE) and the sample quality. |
|
- If `order` == 2, we use DPM-Solver-12 which combines DPM-Solver-1 and singlestep DPM-Solver-2. |
|
- If `order` == 3, we use DPM-Solver-23 which combines singlestep DPM-Solver-2 and singlestep DPM-Solver-3. |
|
===================================================== |
|
Some advices for choosing the algorithm: |
|
- For **unconditional sampling** or **guided sampling with small guidance scale** by DPMs: |
|
Use singlestep DPM-Solver ("DPM-Solver-fast" in the paper) with `order = 3`. |
|
e.g. |
|
>>> dpm_solver = DPM_Solver(model_fn, noise_schedule, predict_x0=False) |
|
>>> x_sample = dpm_solver.sample(x, steps=steps, t_start=t_start, t_end=t_end, order=3, |
|
skip_type='time_uniform', method='singlestep') |
|
- For **guided sampling with large guidance scale** by DPMs: |
|
Use multistep DPM-Solver with `predict_x0 = True` and `order = 2`. |
|
e.g. |
|
>>> dpm_solver = DPM_Solver(model_fn, noise_schedule, predict_x0=True) |
|
>>> x_sample = dpm_solver.sample(x, steps=steps, t_start=t_start, t_end=t_end, order=2, |
|
skip_type='time_uniform', method='multistep') |
|
We support three types of `skip_type`: |
|
- 'logSNR': uniform logSNR for the time steps. **Recommended for low-resolutional images** |
|
- 'time_uniform': uniform time for the time steps. **Recommended for high-resolutional images**. |
|
- 'time_quadratic': quadratic time for the time steps. |
|
===================================================== |
|
Args: |
|
x: A pytorch tensor. The initial value at time `t_start` |
|
e.g. if `t_start` == T, then `x` is a sample from the standard normal distribution. |
|
steps: A `int`. The total number of function evaluations (NFE). |
|
t_start: A `float`. The starting time of the sampling. |
|
If `T` is None, we use self.noise_schedule.T (default is 1.0). |
|
t_end: A `float`. The ending time of the sampling. |
|
If `t_end` is None, we use 1. / self.noise_schedule.total_N. |
|
e.g. if total_N == 1000, we have `t_end` == 1e-3. |
|
For discrete-time DPMs: |
|
- We recommend `t_end` == 1. / self.noise_schedule.total_N. |
|
For continuous-time DPMs: |
|
- We recommend `t_end` == 1e-3 when `steps` <= 15; and `t_end` == 1e-4 when `steps` > 15. |
|
order: A `int`. The order of DPM-Solver. |
|
skip_type: A `str`. The type for the spacing of the time steps. 'time_uniform' or 'logSNR' or 'time_quadratic'. |
|
method: A `str`. The method for sampling. 'singlestep' or 'multistep' or 'singlestep_fixed' or 'adaptive'. |
|
denoise_to_zero: A `bool`. Whether to denoise to time 0 at the final step. |
|
Default is `False`. If `denoise_to_zero` is `True`, the total NFE is (`steps` + 1). |
|
This trick is firstly proposed by DDPM (https://arxiv.org/abs/2006.11239) and |
|
score_sde (https://arxiv.org/abs/2011.13456). Such trick can improve the FID |
|
for diffusion models sampling by diffusion SDEs for low-resolutional images |
|
(such as CIFAR-10). However, we observed that such trick does not matter for |
|
high-resolutional images. As it needs an additional NFE, we do not recommend |
|
it for high-resolutional images. |
|
lower_order_final: A `bool`. Whether to use lower order solvers at the final steps. |
|
Only valid for `method=multistep` and `steps < 15`. We empirically find that |
|
this trick is a key to stabilizing the sampling by DPM-Solver with very few steps |
|
(especially for steps <= 10). So we recommend to set it to be `True`. |
|
solver_type: A `str`. The taylor expansion type for the solver. `dpm_solver` or `taylor`. We recommend `dpm_solver`. |
|
atol: A `float`. The absolute tolerance of the adaptive step size solver. Valid when `method` == 'adaptive'. |
|
rtol: A `float`. The relative tolerance of the adaptive step size solver. Valid when `method` == 'adaptive'. |
|
Returns: |
|
x_end: A pytorch tensor. The approximated solution at time `t_end`. |
|
""" |
|
t_0 = 1. / self.noise_schedule.total_N if t_end is None else t_end |
|
t_T = self.noise_schedule.T if t_start is None else t_start |
|
device = x.device |
|
if method == 'adaptive': |
|
with torch.no_grad(): |
|
x = self.dpm_solver_adaptive(x, order=order, t_T=t_T, t_0=t_0, atol=atol, rtol=rtol, |
|
solver_type=solver_type) |
|
elif method == 'multistep': |
|
assert steps >= order |
|
timesteps = self.get_time_steps(skip_type=skip_type, t_T=t_T, t_0=t_0, N=steps, device=device) |
|
assert timesteps.shape[0] - 1 == steps |
|
with torch.no_grad(): |
|
vec_t = timesteps[0].expand((x.shape[0])) |
|
model_prev_list = [self.model_fn(x, vec_t)] |
|
t_prev_list = [vec_t] |
|
|
|
for init_order in tqdm(range(1, order), desc="DPM init order"): |
|
vec_t = timesteps[init_order].expand(x.shape[0]) |
|
x = self.multistep_dpm_solver_update(x, model_prev_list, t_prev_list, vec_t, init_order, |
|
solver_type=solver_type) |
|
model_prev_list.append(self.model_fn(x, vec_t)) |
|
t_prev_list.append(vec_t) |
|
|
|
for step in tqdm(range(order, steps + 1), desc="DPM multistep"): |
|
vec_t = timesteps[step].expand(x.shape[0]) |
|
if lower_order_final and steps < 15: |
|
step_order = min(order, steps + 1 - step) |
|
else: |
|
step_order = order |
|
x = self.multistep_dpm_solver_update(x, model_prev_list, t_prev_list, vec_t, step_order, |
|
solver_type=solver_type) |
|
for i in range(order - 1): |
|
t_prev_list[i] = t_prev_list[i + 1] |
|
model_prev_list[i] = model_prev_list[i + 1] |
|
t_prev_list[-1] = vec_t |
|
|
|
if step < steps: |
|
model_prev_list[-1] = self.model_fn(x, vec_t) |
|
elif method in ['singlestep', 'singlestep_fixed']: |
|
if method == 'singlestep': |
|
timesteps_outer, orders = self.get_orders_and_timesteps_for_singlestep_solver(steps=steps, order=order, |
|
skip_type=skip_type, |
|
t_T=t_T, t_0=t_0, |
|
device=device) |
|
elif method == 'singlestep_fixed': |
|
K = steps // order |
|
orders = [order, ] * K |
|
timesteps_outer = self.get_time_steps(skip_type=skip_type, t_T=t_T, t_0=t_0, N=K, device=device) |
|
for i, order in enumerate(orders): |
|
t_T_inner, t_0_inner = timesteps_outer[i], timesteps_outer[i + 1] |
|
timesteps_inner = self.get_time_steps(skip_type=skip_type, t_T=t_T_inner.item(), t_0=t_0_inner.item(), |
|
N=order, device=device) |
|
lambda_inner = self.noise_schedule.marginal_lambda(timesteps_inner) |
|
vec_s, vec_t = t_T_inner.tile(x.shape[0]), t_0_inner.tile(x.shape[0]) |
|
h = lambda_inner[-1] - lambda_inner[0] |
|
r1 = None if order <= 1 else (lambda_inner[1] - lambda_inner[0]) / h |
|
r2 = None if order <= 2 else (lambda_inner[2] - lambda_inner[0]) / h |
|
x = self.singlestep_dpm_solver_update(x, vec_s, vec_t, order, solver_type=solver_type, r1=r1, r2=r2) |
|
if denoise_to_zero: |
|
x = self.denoise_to_zero_fn(x, torch.ones((x.shape[0],)).to(device) * t_0) |
|
return x |
|
|
|
|
|
|
|
|
|
|
|
|
|
def interpolate_fn(x, xp, yp): |
|
""" |
|
A piecewise linear function y = f(x), using xp and yp as keypoints. |
|
We implement f(x) in a differentiable way (i.e. applicable for autograd). |
|
The function f(x) is well-defined for all x-axis. (For x beyond the bounds of xp, we use the outmost points of xp to define the linear function.) |
|
Args: |
|
x: PyTorch tensor with shape [N, C], where N is the batch size, C is the number of channels (we use C = 1 for DPM-Solver). |
|
xp: PyTorch tensor with shape [C, K], where K is the number of keypoints. |
|
yp: PyTorch tensor with shape [C, K]. |
|
Returns: |
|
The function values f(x), with shape [N, C]. |
|
""" |
|
N, K = x.shape[0], xp.shape[1] |
|
all_x = torch.cat([x.unsqueeze(2), xp.unsqueeze(0).repeat((N, 1, 1))], dim=2) |
|
sorted_all_x, x_indices = torch.sort(all_x, dim=2) |
|
x_idx = torch.argmin(x_indices, dim=2) |
|
cand_start_idx = x_idx - 1 |
|
start_idx = torch.where( |
|
torch.eq(x_idx, 0), |
|
torch.tensor(1, device=x.device), |
|
torch.where( |
|
torch.eq(x_idx, K), torch.tensor(K - 2, device=x.device), cand_start_idx, |
|
), |
|
) |
|
end_idx = torch.where(torch.eq(start_idx, cand_start_idx), start_idx + 2, start_idx + 1) |
|
start_x = torch.gather(sorted_all_x, dim=2, index=start_idx.unsqueeze(2)).squeeze(2) |
|
end_x = torch.gather(sorted_all_x, dim=2, index=end_idx.unsqueeze(2)).squeeze(2) |
|
start_idx2 = torch.where( |
|
torch.eq(x_idx, 0), |
|
torch.tensor(0, device=x.device), |
|
torch.where( |
|
torch.eq(x_idx, K), torch.tensor(K - 2, device=x.device), cand_start_idx, |
|
), |
|
) |
|
y_positions_expanded = yp.unsqueeze(0).expand(N, -1, -1) |
|
start_y = torch.gather(y_positions_expanded, dim=2, index=start_idx2.unsqueeze(2)).squeeze(2) |
|
end_y = torch.gather(y_positions_expanded, dim=2, index=(start_idx2 + 1).unsqueeze(2)).squeeze(2) |
|
cand = start_y + (x - start_x) * (end_y - start_y) / (end_x - start_x) |
|
return cand |
|
|
|
|
|
def expand_dims(v, dims): |
|
""" |
|
Expand the tensor `v` to the dim `dims`. |
|
Args: |
|
`v`: a PyTorch tensor with shape [N]. |
|
`dim`: a `int`. |
|
Returns: |
|
a PyTorch tensor with shape [N, 1, 1, ..., 1] and the total dimension is `dims`. |
|
""" |
|
return v[(...,) + (None,) * (dims - 1)] |