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| # SPDX-License-Identifier: Apache-2.0 | |
| # | |
| # Independent reimplementation of standard sinusoidal position- and | |
| # timestep-embedding utilities, written from their public mathematical | |
| # definitions (see the per-symbol references below). This file is NOT derived | |
| # from the DiT source tree and carries no third-party (CC BY-NC) copyright; it | |
| # is released under Apache-2.0 like the rest of this package. | |
| # | |
| # References for the underlying formulas (math only, no code reuse): | |
| # * Sinusoidal position encoding — Vaswani et al., "Attention Is All You | |
| # Need" (2017), Section 3.5. | |
| # * Sinusoidal timestep embedding — Ho et al., "Denoising Diffusion | |
| # Probabilistic Models" (2020); the same closed form is reused across | |
| # diffusion and flow-matching models. | |
| # | |
| # The module layout, parameter names, and numerical outputs are intentionally | |
| # identical to the previous version so that existing checkpoints load unchanged | |
| # and inference results are bit-for-bit reproducible. | |
| import math | |
| import numpy as np | |
| import torch | |
| from torch import nn | |
| # --------------------------------------------------------------------------- # | |
| # Sinusoidal (sin-cos) position embeddings | |
| # | |
| # For a position p and channel index i the embedding interleaves | |
| # sin(p / 10000^(2i/d)) and cos(p / 10000^(2i/d)), | |
| # i.e. the classic Transformer positional encoding. The 2D variant encodes the | |
| # height and width axes with half the channels each and concatenates them. | |
| # --------------------------------------------------------------------------- # | |
| def get_1d_sincos_pos_embed_from_grid(embed_dim, pos): | |
| """1D sin-cos embedding for a flat array of positions. | |
| Args: | |
| embed_dim: even output dimension per position. | |
| pos: array of positions, any shape; flattened to (M,). | |
| Returns: | |
| (M, embed_dim) array, [sin | cos] halves concatenated. | |
| """ | |
| assert embed_dim % 2 == 0 | |
| # Inverse frequencies 1 / 10000^(k/(embed_dim/2)) for k = 0 .. embed_dim/2-1. | |
| inv_freq = np.arange(embed_dim // 2, dtype=np.float64) | |
| inv_freq /= embed_dim / 2.0 | |
| inv_freq = 1.0 / 10000**inv_freq # (embed_dim/2,) | |
| angles = np.einsum("m,d->md", pos.reshape(-1), inv_freq) # outer product (M, D/2) | |
| return np.concatenate([np.sin(angles), np.cos(angles)], axis=1) # (M, D) | |
| def get_2d_sincos_pos_embed_from_grid(embed_dim, grid): | |
| """2D sin-cos embedding: half the channels encode each spatial axis.""" | |
| assert embed_dim % 2 == 0 | |
| emb_h = get_1d_sincos_pos_embed_from_grid(embed_dim // 2, grid[0]) # (H*W, D/2) | |
| emb_w = get_1d_sincos_pos_embed_from_grid(embed_dim // 2, grid[1]) # (H*W, D/2) | |
| return np.concatenate([emb_h, emb_w], axis=1) # (H*W, D) | |
| def get_2d_sincos_pos_embed(embed_dim, grid_size, cls_token=False, extra_tokens=0): | |
| """Sin-cos table for a ``grid_size x grid_size`` patch grid. | |
| Returns an ``(grid_size**2 [+ extra_tokens], embed_dim)`` array. When | |
| ``cls_token`` is set and ``extra_tokens > 0``, that many zero rows are | |
| prepended. | |
| """ | |
| axis_h = np.arange(grid_size, dtype=np.float32) | |
| axis_w = np.arange(grid_size, dtype=np.float32) | |
| grid = np.meshgrid(axis_w, axis_h) # width varies fastest | |
| grid = np.stack(grid, axis=0).reshape([2, 1, grid_size, grid_size]) | |
| pos_embed = get_2d_sincos_pos_embed_from_grid(embed_dim, grid) | |
| if cls_token and extra_tokens > 0: | |
| pos_embed = np.concatenate([np.zeros([extra_tokens, embed_dim]), pos_embed], axis=0) | |
| return pos_embed | |
| # --------------------------------------------------------------------------- # | |
| # Timestep embedding | |
| # --------------------------------------------------------------------------- # | |
| class TimestepEmbedder(nn.Module): | |
| """Embed scalar (possibly fractional) timesteps into vectors. | |
| Sinusoidal frequency features are fed through a two-layer MLP with a SiLU | |
| non-linearity. This is the standard timestep conditioning used by diffusion | |
| and flow-matching models. | |
| """ | |
| def __init__(self, hidden_size, frequency_embedding_size=256): | |
| super().__init__() | |
| self.mlp = nn.Sequential( | |
| nn.Linear(frequency_embedding_size, hidden_size, bias=True), | |
| nn.SiLU(), | |
| nn.Linear(hidden_size, hidden_size, bias=True), | |
| ) | |
| self.frequency_embedding_size = frequency_embedding_size | |
| def timestep_embedding(t, dim, max_period=10000): | |
| """Sinusoidal features for a 1D tensor of (possibly fractional) timesteps. | |
| Args: | |
| t: (N,) tensor of timestep values. | |
| dim: output feature dimension. | |
| max_period: lowest angular frequency (longest period). | |
| Returns: | |
| (N, dim) tensor of [cos | sin] features (zero-padded if ``dim`` is odd). | |
| """ | |
| half = dim // 2 | |
| # Geometrically spaced frequencies over [1, 1/max_period]. | |
| freqs = torch.exp( | |
| -math.log(max_period) * torch.arange(start=0, end=half, dtype=torch.float32) / half | |
| ).to(device=t.device) | |
| args = t[:, None].float() * freqs[None] | |
| embedding = torch.cat([torch.cos(args), torch.sin(args)], dim=-1) | |
| if dim % 2: | |
| embedding = torch.cat([embedding, torch.zeros_like(embedding[:, :1])], dim=-1) | |
| return embedding | |
| def forward(self, t): | |
| freq_features = self.timestep_embedding(t, self.frequency_embedding_size) | |
| freq_features = freq_features.to(next(self.mlp.parameters()).dtype) | |
| return self.mlp(freq_features) | |
| class PositionEmbedding(nn.Module): | |
| """Fixed 2D sin-cos position table exposed as a lookup by position id.""" | |
| def __init__(self, max_num_patch_per_side, hidden_size): | |
| super().__init__() | |
| self.max_num_patch_per_side = max_num_patch_per_side | |
| self.hidden_size = hidden_size | |
| # Build the (non-trainable) table eagerly. If it were created lazily it | |
| # could stay on the meta device through transformers' | |
| # from_pretrained(dtype=...) path and later materialize as uninitialized | |
| # memory when moved to the GPU. | |
| table = get_2d_sincos_pos_embed(hidden_size, max_num_patch_per_side) | |
| self.pos_embed = nn.Parameter( | |
| torch.from_numpy(table).float(), | |
| requires_grad=False, | |
| ) | |
| def _reset_parameters(self): | |
| """Recompute the table after a meta-init path (call post-from_pretrained).""" | |
| table = get_2d_sincos_pos_embed(self.hidden_size, self.max_num_patch_per_side) | |
| on_meta = self.pos_embed.is_meta or self.pos_embed.device.type == "meta" | |
| materialized = torch.from_numpy(table).to( | |
| device="cpu" if on_meta else self.pos_embed.device, | |
| dtype=torch.float32 if on_meta else self.pos_embed.dtype, | |
| ) | |
| if on_meta: | |
| self.pos_embed = nn.Parameter(materialized.float(), requires_grad=False) | |
| else: | |
| self.pos_embed.data.copy_(materialized.to(self.pos_embed.dtype)) | |
| def forward(self, position_ids): | |
| return self.pos_embed[position_ids] | |