import math import torch from torch import nn import torchsde from tqdm.auto import trange, tqdm import comfy.sample import k_diffusion.sampling from k_diffusion.sampling import BrownianTreeNoiseSampler, PIDStepSizeController, get_ancestral_step, to_d, default_noise_sampler import random # The following function adds the samplers during initialization, in __init__.py def add_samplers(): from comfy.samplers import KSampler, k_diffusion_sampling if hasattr(KSampler, "DISCARD_PENULTIMATE_SIGMA_SAMPLERS"): KSampler.DISCARD_PENULTIMATE_SIGMA_SAMPLERS |= discard_penultimate_sigma_samplers added = 0 for sampler in extra_samplers: #getattr(self, "sample_{}".format(extra_samplers)) if sampler not in KSampler.SAMPLERS: try: idx = KSampler.SAMPLERS.index("uni_pc_bh2") # Last item in the samplers list KSampler.SAMPLERS.insert(idx+1, sampler) # Add our custom samplers setattr(k_diffusion_sampling, "sample_{}".format(sampler), extra_samplers[sampler]) added += 1 except ValueError as _err: pass if added > 0: import importlib importlib.reload(k_diffusion_sampling) # The following function adds the samplers during initialization, in __init__.py def add_schedulers(): from comfy.samplers import KSampler, k_diffusion_sampling for scheduler in extra_schedulers: #getattr(self, "sample_{}".format(extra_samplers)) if scheduler not in KSampler.SCHEDULERS: try: idx = KSampler.SCHEDULERS.index("ddim_uniform") # Last item in the samplers list KSampler.SCHEDULERS.insert(idx+1, scheduler) # Add our custom samplers setattr(k_diffusion_sampling, "get_sigmas_{}".format(scheduler), extra_schedulers[scheduler]) import importlib importlib.reload(k_diffusion_sampling) except ValueError as err: pass # Noise samplers from torch import Generator, Tensor, lerp from torch.nn.functional import unfold from typing import Callable, Tuple from math import pi def get_positions(block_shape: Tuple[int, int]) -> Tensor: """ Generate position tensor. Arguments: block_shape -- (height, width) of position tensor Returns: position vector shaped (1, height, width, 1, 1, 2) """ bh, bw = block_shape positions = torch.stack( torch.meshgrid( [(torch.arange(b) + 0.5) / b for b in (bw, bh)], indexing="xy", ), -1, ).view(1, bh, bw, 1, 1, 2) return positions def unfold_grid(vectors: Tensor) -> Tensor: """ Unfold vector grid to batched vectors. Arguments: vectors -- grid vectors Returns: batched grid vectors """ batch_size, _, gpy, gpx = vectors.shape return ( unfold(vectors, (2, 2)) .view(batch_size, 2, 4, -1) .permute(0, 2, 3, 1) .view(batch_size, 4, gpy - 1, gpx - 1, 2) ) def smooth_step(t: Tensor) -> Tensor: """ Smooth step function [0, 1] -> [0, 1]. Arguments: t -- input values (any shape) Returns: output values (same shape as input values) """ return t * t * (3.0 - 2.0 * t) def perlin_noise_tensor( vectors: Tensor, positions: Tensor, step: Callable = None ) -> Tensor: """ Generate perlin noise from batched vectors and positions. Arguments: vectors -- batched grid vectors shaped (batch_size, 4, grid_height, grid_width, 2) positions -- batched grid positions shaped (batch_size or 1, block_height, block_width, grid_height or 1, grid_width or 1, 2) Keyword Arguments: step -- smooth step function [0, 1] -> [0, 1] (default: `smooth_step`) Raises: Exception: if position and vector shapes do not match Returns: (batch_size, block_height * grid_height, block_width * grid_width) """ if step is None: step = smooth_step batch_size = vectors.shape[0] # grid height, grid width gh, gw = vectors.shape[2:4] # block height, block width bh, bw = positions.shape[1:3] for i in range(2): if positions.shape[i + 3] not in (1, vectors.shape[i + 2]): raise Exception( f"Blocks shapes do not match: vectors ({vectors.shape[1]}, {vectors.shape[2]}), positions {gh}, {gw})" ) if positions.shape[0] not in (1, batch_size): raise Exception( f"Batch sizes do not match: vectors ({vectors.shape[0]}), positions ({positions.shape[0]})" ) vectors = vectors.view(batch_size, 4, 1, gh * gw, 2) positions = positions.view(positions.shape[0], bh * bw, -1, 2) step_x = step(positions[..., 0]) step_y = step(positions[..., 1]) row0 = lerp( (vectors[:, 0] * positions).sum(dim=-1), (vectors[:, 1] * (positions - positions.new_tensor((1, 0)))).sum(dim=-1), step_x, ) row1 = lerp( (vectors[:, 2] * (positions - positions.new_tensor((0, 1)))).sum(dim=-1), (vectors[:, 3] * (positions - positions.new_tensor((1, 1)))).sum(dim=-1), step_x, ) noise = lerp(row0, row1, step_y) return ( noise.view( batch_size, bh, bw, gh, gw, ) .permute(0, 3, 1, 4, 2) .reshape(batch_size, gh * bh, gw * bw) ) def perlin_noise( grid_shape: Tuple[int, int], out_shape: Tuple[int, int], batch_size: int = 1, generator: Generator = None, *args, **kwargs, ) -> Tensor: """ Generate perlin noise with given shape. `*args` and `**kwargs` are forwarded to `Tensor` creation. Arguments: grid_shape -- Shape of grid (height, width). out_shape -- Shape of output noise image (height, width). Keyword Arguments: batch_size -- (default: {1}) generator -- random generator used for grid vectors (default: {None}) Raises: Exception: if grid and out shapes do not match Returns: Noise image shaped (batch_size, height, width) """ # grid height and width gh, gw = grid_shape # output height and width oh, ow = out_shape # block height and width bh, bw = oh // gh, ow // gw if oh != bh * gh: raise Exception(f"Output height {oh} must be divisible by grid height {gh}") if ow != bw * gw != 0: raise Exception(f"Output width {ow} must be divisible by grid width {gw}") angle = torch.empty( [batch_size] + [s + 1 for s in grid_shape], *args, **kwargs ).uniform_(to=2.0 * pi, generator=generator) # random vectors on grid points vectors = unfold_grid(torch.stack((torch.cos(angle), torch.sin(angle)), dim=1)) # positions inside grid cells [0, 1) positions = get_positions((bh, bw)).to(vectors) return perlin_noise_tensor(vectors, positions).squeeze(0) def rand_perlin_like(x): noise = torch.randn_like(x) / 2.0 noise_size_H = noise.size(dim=2) noise_size_W = noise.size(dim=3) perlin = None for i in range(2): noise += perlin_noise((noise_size_H, noise_size_W), (noise_size_H, noise_size_W), batch_size=4).to(x.device) #noise += perlin #print(noise) return noise / noise.std() def uniform_noise_sampler(x): # Even distribution, seemingly produces more information in non-subject areas than the normal (gaussian) noise sampler return lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 from torch.distributions import StudentT def studentt_noise_sampler(x): # Produces more subject-focused outputs due to distribution, unsure if this works noise = StudentT(loc=0, scale=0.2, df=1).rsample(x.size()) #noise *= 2 / (torch.max(torch.abs(noise)) + 1e-8) s: FloatTensor = torch.quantile( noise.flatten(start_dim=1).abs(), 0.75, dim = -1 ) #s.clamp_(min = 1.) s = s.reshape(*s.shape, 1, 1, 1) noise = noise.clamp(-s, s) noise = torch.copysign(torch.pow(torch.abs(noise), 0.5), noise) print(s) return lambda sigma, sigma_next: noise.to(x.device) / (7/3) from torch.distributions import Laplace def rand_laplacian_like(x): noise = torch.randn_like(x) / 4.0 noise_size_H = noise.size(dim=2) noise_size_W = noise.size(dim=3) noise += Laplace(loc=0, scale=1.0).rsample(x.size()).to(noise.device) #noise += perlin #print(noise) return noise / noise.std() def highres_pyramid_noise_like(x, discount=0.7): b, c, h, w = x.shape # EDIT: w and h get over-written, rename for a different variant! orig_h = h orig_w = w u = torch.nn.Upsample(size=(orig_h, orig_w), mode='bilinear') noise = (torch.rand_like(x) - 0.5) * 2 * 1.73 # Start with scaled uniform noise for i in range(4): r = random.random()*2+2 # Rather than always going 2x, h, w = min(orig_h*15, int(h*(r**i))), min(orig_w*15, int(w*(r**i))) noise += u(torch.randn(b, c, h, w).to(x)) * discount**i if h>=orig_h*15 or w>=orig_w*15: break # Lowest resolution is 1x1 return noise/noise.std() # Scaled back to roughly unit variance def green_noise_like(x): noise = torch.randn_like(x) width = noise.size(dim=2) height = noise.size(dim=3) scale = 1.0 / (width * height) fy = torch.fft.fftfreq(width, device=x.device)[:, None] ** 2 fx = torch.fft.fftfreq(height, device=x.device) ** 2 f = fy + fx power = torch.sqrt(f) power[0, 0] = 1 noise = torch.fft.ifft2(torch.fft.fft2(noise) / torch.sqrt(power)) noise *= scale / noise.std() noise = torch.real(noise).to(x.device) return noise / noise.std() def green_noise_sampler(x): # This doesn't work properly right now width = x.size(dim=2) height = x.size(dim=3) noise = torch.randn(width, height) #scale = 1.0 / (width * height) fy = torch.fft.fftfreq(width)[:, None] ** 2 fx = torch.fft.fftfreq(height) ** 2 f = fy + fx power = torch.sqrt(f) power[0, 0] = 1 noise = torch.fft.ifft2(torch.fft.fft2(noise) / torch.sqrt(power)) #noise *= scale / noise.std() noise = torch.real(noise).to(x.device) mean = torch.mean(noise) std = torch.std(noise) noise.sub_(mean).div_(std) print(noise) return lambda sigma, sigma_next: noise def power_noise_sampler(tensor, alpha=2, k=1): # This doesn't work properly right now """Generate 1/f noise for a given tensor. Args: tensor: The tensor to add noise to. alpha: The parameter that determines the slope of the spectrum. k: A constant. Returns: A tensor with the same shape as `tensor` containing 1/f noise. """ tensor = torch.randn_like(tensor) fft = torch.fft.fft2(tensor) freq = torch.arange(1, len(fft) + 1, dtype=torch.float) spectral_density = k / freq**alpha noise = torch.rand(tensor.shape) * spectral_density mean = torch.mean(noise, dim=(-2, -1), keepdim=True).to(tensor.device) std = torch.std(noise, dim=(-2, -1), keepdim=True).to(tensor.device) noise = noise.to(tensor.device).sub_(mean).div_(std) variance = torch.var(noise, dim=(-2, -1), keepdim=True) print(variance) return lambda sigma, sigma_next: noise / 3 # Below this point are extra samplers @torch.no_grad() def sample_clyb_4m_sde_momentumized(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1.0, s_noise=1., noise_sampler=None, momentum=0.0): """DPM-Solver++(3M) SDE, modified with an extra SDE, and momentumized in both the SDE and ODE(?). 'its a first' - Clybius 2023 The expression for d1 is derived from the extrapolation formula given in the paper “Diffusion Monte Carlo with stochastic Hamiltonians” by M. Foulkes, L. Mitas, R. Needs, and G. Rajagopal. The formula is given as follows: d1 = d1_0 + (d1_0 - d1_1) * r2 / (r2 + r1) + ((d1_0 - d1_1) * r2 / (r2 + r1) - (d1_1 - d1_2) * r1 / (r0 + r1)) * r2 / ((r2 + r1) * (r0 + r1)) (if this is an incorrect citing, we blame Google's Bard and OpenAI's ChatGPT for this and NOT me :^) ) where d1_0, d1_1, and d1_2 are defined as follows: d1_0 = (denoised - denoised_1) / r2 d1_1 = (denoised_1 - denoised_2) / r1 d1_2 = (denoised_2 - denoised_3) / r0 The variables r0, r1, and r2 are defined as follows: r0 = h_3 / h_2 r1 = h_2 / h r2 = h / h_1 """ def momentum_func(diff, velocity, timescale=1.0, offset=-momentum / 2.0): # Diff is current diff, vel is previous diff if velocity is None: momentum_vel = diff else: momentum_vel = momentum * (timescale + offset) * velocity + (1 - momentum * (timescale + offset)) * diff return momentum_vel sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() noise_sampler = rand_perlin_like(x) if noise_sampler is None else noise_sampler extra_args = {} if extra_args is None else extra_args s_in = x.new_ones([x.shape[0]]) denoised_1, denoised_2, denoised_3 = None, None, None h_1, h_2, h_3 = None, None, None vel, vel_sde = None, None for i in trange(len(sigmas) - 1, disable=disable): time = sigmas[i] / sigma_max denoised = model(x, sigmas[i] * s_in, **extra_args) if callback is not None: callback({'x': x, 'i': i, 'sigma': sigmas[i], 'sigma_hat': sigmas[i], 'denoised': denoised}) if sigmas[i + 1] == 0: # Denoising step x = denoised else: t, s = -sigmas[i].log(), -sigmas[i + 1].log() h = s - t h_eta = h * (eta + 1) x_diff = momentum_func((-h_eta).expm1().neg() * denoised, vel, time) vel = x_diff x = torch.exp(-h_eta) * x + vel if h_3 is not None: r0 = h_3 / h_2 r1 = h_2 / h r2 = h / h_1 d1_0 = (denoised - denoised_1) / r2 d1_1 = (denoised_1 - denoised_2) / r1 d1_2 = (denoised_2 - denoised_3) / r0 d1 = d1_0 + (d1_0 - d1_1) * r2 / (r2 + r1) + ((d1_0 - d1_1) * r2 / (r2 + r1) - (d1_1 - d1_2) * r1 / (r0 + r1)) * r2 / ((r2 + r1) * (r0 + r1)) d2 = (d1_0 - d1_1) / (r2 + r1) + ((d1_0 - d1_1) * r2 / (r2 + r1) - (d1_1 - d1_2) * r1 / (r0 + r1)) / ((r2 + r1) * (r0 + r1)) phi_3 = h_eta.neg().expm1() / h_eta + 1 phi_4 = phi_3 / h_eta - 0.5 sde_diff = momentum_func(phi_3 * d1 - phi_4 * d2, vel_sde, time) vel_sde = sde_diff x = x + vel_sde elif h_2 is not None: r0 = h_1 / h r1 = h_2 / h d1_0 = (denoised - denoised_1) / r0 d1_1 = (denoised_1 - denoised_2) / r1 d1 = d1_0 + (d1_0 - d1_1) * r0 / (r0 + r1) d2 = (d1_0 - d1_1) / (r0 + r1) phi_2 = h_eta.neg().expm1() / h_eta + 1 phi_3 = phi_2 / h_eta - 0.5 sde_diff = momentum_func(phi_2 * d1 - phi_3 * d2, vel_sde, time) vel_sde = sde_diff x = x + vel_sde elif h_1 is not None: r = h_1 / h d = (denoised - denoised_1) / r phi_2 = h_eta.neg().expm1() / h_eta + 1 sde_diff = momentum_func(phi_2 * d, vel_sde, time) vel_sde = sde_diff x = x + vel_sde if eta: x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * sigmas[i + 1] * (-2 * h * eta).expm1().neg().sqrt() * s_noise denoised_1, denoised_2, denoised_3 = denoised, denoised_1, denoised_2 h_1, h_2, h_3 = h, h_1, h_2 return x # Kat's Truncated Taylor Method sampler, by Katherine Crowson def sample_ttm_jvp(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler=None): """Second order truncated Taylor method (torch.func.jvp() version).""" extra_args = {} if extra_args is None else extra_args noise_sampler = default_noise_sampler(x) if noise_sampler is None else noise_sampler s_in = x.new_ones([x.shape[0]]) model_fn = lambda x, sigma: model(x, sigma * s_in, **extra_args) for i in trange(len(sigmas) - 1, disable=disable): denoised = model_fn(x, sigmas[i]) if callback is not None: callback({'x': x, 'i': i, 'sigma': sigmas[i], 'sigma_hat': sigmas[i], 'denoised': denoised}) if sigmas[i + 1] == 0: # Denoising step x = denoised else: # 2nd order truncated Taylor method t, s = -sigmas[i].log(), -sigmas[i + 1].log() h = s - t h_eta = h * (eta + 1) eps = to_d(x, sigmas[i], denoised) _, denoised_prime = torch.func.jvp(model_fn, (x, sigmas[i]), (eps * -sigmas[i], -sigmas[i])) phi_1 = -torch.expm1(-h_eta) #phi_2 = torch.expm1(-h_eta) + h_eta phi_2 = torch.expm1(-h) + h # seems to work better with eta > 0 x = torch.exp(-h_eta) * x + phi_1 * denoised + phi_2 * denoised_prime if eta: phi_1_noise = torch.sqrt(-torch.expm1(-2 * h * eta)) x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * sigmas[i + 1] * phi_1_noise * s_noise return x # Many thanks to Kat + Birch-San for this wonderful sampler implementation! https://github.com/Birch-san/sdxl-play/commits/res/ from .other_samplers.refined_exp_solver import sample_refined_exp_s def sample_res_solver(model, x, sigmas, extra_args=None, callback=None, disable=None, noise_sampler=None, denoise_to_zero=True, simple_phi_calc=False, c2=0.5, ita=torch.Tensor((0.25,)), momentum=0.0): sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() seed = extra_args.get("seed", None) match noise_sampler: case "brownian": noise_sampler = BrownianTreeNoiseSampler(x, sigma_min, sigma_max, seed=seed, cpu=False) case "gaussian": noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) case "uniform": noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 case "highres-pyramid": noise_sampler = lambda sigma, sigma_next: highres_pyramid_noise_like(x) case "perlin": noise_sampler = lambda sigma, sigma_next: rand_perlin_like(x) case "laplacian": noise_sampler = lambda sigma, sigma_next: rand_laplacian_like(x) case _: noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) return sample_refined_exp_s(model, x, sigmas, extra_args=extra_args, callback=callback, disable=disable, noise_sampler=noise_sampler, denoise_to_zero=denoise_to_zero, simple_phi_calc=simple_phi_calc, c2=c2, ita=ita, momentum=momentum) @torch.no_grad() def sample_dpmpp_dualsde_momentum(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler=None, r=1/2, momentum=0.0): """DPM-Solver++ (Stochastic with Momentum). Personal modified sampler by Clybius""" sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() noise_sampler = rand_perlin_like(x) if noise_sampler is None else noise_sampler extra_args = {} if extra_args is None else extra_args s_in = x.new_ones([x.shape[0]]) sigma_fn = lambda t: t.neg().exp() t_fn = lambda sigma: sigma.log().neg() denoisedsde_1, denoisedsde_2, denoisedsde_3 = None, None, None # new line h_1, h_2, h_3 = None, None, None # new line def momentum_func(diff, velocity, timescale=1.0, offset=-momentum / 2.0): # Diff is current diff, vel is previous diff if velocity is None: momentum_vel = diff else: momentum_vel = momentum * (timescale + offset) * velocity + (1 - momentum * (timescale + offset)) * diff return momentum_vel vel = None vel_2 = None vel_sde = None for i in trange(len(sigmas) - 1, disable=disable): time = sigmas[i] / sigma_max denoised = model(x, sigmas[i] * s_in, **extra_args) if callback is not None: callback({'x': x, 'i': i, 'sigma': sigmas[i], 'sigma_hat': sigmas[i], 'denoised': denoised}) if sigmas[i + 1] == 0: # Euler method d = to_d(x, sigmas[i], denoised) dt = sigmas[i + 1] - sigmas[i] x = x + d * dt else: # DPM-Solver++ t, t_next = t_fn(sigmas[i]), t_fn(sigmas[i + 1]) h = t_next - t h_eta = h * (eta + 1) s = t + h * r fac = 1 / (2 * r) # Step 1 sd, su = get_ancestral_step(sigma_fn(t), sigma_fn(s), eta) s_ = t_fn(sd) diff_2 = momentum_func((t - s_).expm1() * denoised, vel_2, time) vel_2 = diff_2 x_2 = (sigma_fn(s_) / sigma_fn(t)) * x - diff_2 x_2 = x_2 + noise_sampler(sigma_fn(t), sigma_fn(s)) * s_noise * su denoised_2 = model(x_2, sigma_fn(s) * s_in, **extra_args) # Step 2 sd, su = get_ancestral_step(sigma_fn(t), sigma_fn(t_next), eta) t_next_ = t_fn(sd) denoised_d = (1 - fac) * denoised + fac * denoised_2 diff = momentum_func((t - t_next_).expm1() * denoised_d, vel, time) vel = diff x = (sigma_fn(t_next_) / sigma_fn(t)) * x - diff if h_3 is not None: r0 = h_3 / h_2 r1 = h_2 / h r2 = h / h_1 d1_0 = (denoised_d - denoisedsde_1) / r2 d1_1 = (denoisedsde_1 - denoisedsde_2) / r1 d1_2 = (denoisedsde_2 - denoisedsde_3) / r0 d1 = d1_0 + (d1_0 - d1_1) * r2 / (r2 + r1) + ((d1_0 - d1_1) * r2 / (r2 + r1) - (d1_1 - d1_2) * r1 / (r0 + r1)) * r2 / ((r2 + r1) * (r0 + r1)) d2 = (d1_0 - d1_1) / (r2 + r1) + ((d1_0 - d1_1) * r2 / (r2 + r1) - (d1_1 - d1_2) * r1 / (r0 + r1)) / ((r2 + r1) * (r0 + r1)) phi_3 = h_eta.neg().expm1() / h_eta + 1 phi_4 = phi_3 / h_eta - 0.5 diff = momentum_func(phi_3 * d1 - phi_4 * d2, vel_sde, time) vel_sde = diff x = x + diff elif h_2 is not None: r0 = h_1 / h r1 = h_2 / h d1_0 = (denoised_d - denoisedsde_1) / r0 d1_1 = (denoisedsde_1 - denoisedsde_2) / r1 d1 = d1_0 + (d1_0 - d1_1) * r0 / (r0 + r1) d2 = (d1_0 - d1_1) / (r0 + r1) phi_2 = h_eta.neg().expm1() / h_eta + 1 phi_3 = phi_2 / h_eta - 0.5 diff = momentum_func(phi_2 * d1 - phi_3 * d2, vel_sde, time) vel_sde = diff x = x + diff elif h_1 is not None: r = h_1 / h d = (denoised_d - denoisedsde_1) / r phi_2 = h_eta.neg().expm1() / h_eta + 1 diff = momentum_func(phi_2 * d, vel_sde, time) vel_sde = diff x = x + diff if eta: x = x + noise_sampler(sigma_fn(t), sigma_fn(t_next)) * s_noise * su #if 'denoised_d' in locals(): denoisedsde_1, denoisedsde_2, denoisedsde_3 = denoised_d, denoisedsde_1, denoisedsde_2 # new line #if 'h' in locals(): h_1, h_2, h_3 = h, h_1, h_2 return x def sample_dpmpp_dualsdemomentum(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler=None, r=1/2, momentum=0.0): sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() seed = extra_args.get("seed", None) match noise_sampler: case "brownian": noise_sampler = BrownianTreeNoiseSampler(x, sigma_min, sigma_max, seed=seed, cpu=False) case "gaussian": noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) case "uniform": noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 case "perlin": noise_sampler = lambda sigma, sigma_next: rand_perlin_like(x) case "laplacian": noise_sampler = lambda sigma, sigma_next: rand_laplacian_like(x) case _: noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) return sample_dpmpp_dualsde_momentum(model, x, sigmas, extra_args=extra_args, callback=callback, disable=disable, eta=eta, s_noise=s_noise, noise_sampler=noise_sampler, r=r, momentum=momentum) from .other_samplers.sample_ttm import sample_ttm_jvp def sample_ttmcustom(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler=None): sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() seed = extra_args.get("seed", None) match noise_sampler: case "gaussian": noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) case "uniform": noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 case "brownian": noise_sampler = BrownianTreeNoiseSampler(x, sigma_min, sigma_max, seed=seed, cpu=False) case _: noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) return sample_ttm_jvp(model, x, sigmas, extra_args=extra_args, callback=callback, disable=disable, eta=eta, s_noise=s_noise, noise_sampler=noise_sampler) from k_diffusion.sampling import sample_lcm def sample_lcmcustom(model, x, sigmas, extra_args=None, callback=None, disable=None, noise_sampler=None): sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() seed = extra_args.get("seed", None) match noise_sampler: case "gaussian": noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) case "uniform": noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 case "brownian": noise_sampler = BrownianTreeNoiseSampler(x, sigma_min, sigma_max, seed=seed, cpu=False) case _: noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) return sample_lcm(model, x, sigmas, extra_args=extra_args, callback=callback, disable=disable, noise_sampler=noise_sampler) def sample_clyb_4m_sde(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler="brownian", momentum=0.0): sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() seed = extra_args.get("seed", None) match noise_sampler: case "brownian": noise_sampler = BrownianTreeNoiseSampler(x, sigma_min, sigma_max, seed=seed, cpu=False) case "gaussian": noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) case "uniform": noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 case "highres-pyramid": noise_sampler = lambda sigma, sigma_next: highres_pyramid_noise_like(x) case "perlin": noise_sampler = lambda sigma, sigma_next: rand_perlin_like(x) case "laplacian": noise_sampler = lambda sigma, sigma_next: rand_laplacian_like(x) case _: noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 return sample_clyb_4m_sde_momentumized(model, x, sigmas, extra_args=extra_args, callback=callback, disable=disable, eta=eta, s_noise=s_noise, noise_sampler=noise_sampler, momentum=momentum) """ # This code works, but I'm currently experimenting with different methods @torch.no_grad() def sampler_euler_ancestral_dancing(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler=None, leap=2, eta_dance=1.0): #Ancestral sampling with Euler method steps, dancing steps. extra_args = {} if extra_args is None else extra_args noise_sampler = default_noise_sampler(x) if noise_sampler is None else noise_sampler unsample_noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) s_in = x.new_ones([x.shape[0]]) for i in trange(len(sigmas) - 1, disable=disable): if i < len(sigmas) - leap: is_danceable = sigmas[i + leap] > 0 else: is_danceable = False denoised = model(x, sigmas[i] * s_in, **extra_args) sigma_down, sigma_up = get_ancestral_step(sigmas[i], sigmas[i + leap] if is_danceable else sigmas[i + 1], eta=eta) if callback is not None: callback({'x': x, 'i': i, 'sigma': sigmas[i], 'sigma_hat': sigmas[i], 'denoised': denoised}) d = to_d(x, sigmas[i], denoised) # Euler method dt = sigma_down - sigmas[i] x = x + d * dt if sigmas[i + 1] > 0: if is_danceable: x = x + noise_sampler(sigmas[i], sigmas[i + leap]) * s_noise * sigma_up #x = x + noise_sampler(sigmas[i + 2], sigmas[i + 1]) * s_noise * sigma_up #denoised2 = model(x, sigmas[i + 2] * s_in, **extra_args) sigma_down2, sigma_up2 = get_ancestral_step(sigmas[i + leap], sigmas[i + 1], eta=eta_dance) d_2 = to_d(x, sigmas[i + leap], denoised) dt_2 = sigma_down2 - sigmas[i + leap] x = x + d_2 * dt_2 x = x + noise_sampler(sigmas[i + leap], sigmas[i + 1]) * s_noise * sigma_up2 #sigma_down3, sigma_up3 = get_ancestral_step(sigmas[i], sigmas[i + 1], eta=eta) #x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * s_noise * sigma_up3 #denoised2 = model(x, sigmas[i] * s_in, **extra_args) #d_3 = to_d(x, sigmas[i], denoised2) #dt_3 = sigma_down3 - sigmas[i] #x = x + d_3 * dt_3 + d_2 * dt_2 #print(dt_3, dt_2) #x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * s_noise * sigma_up3 #x = x + d * dt else: x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * s_noise * sigma_up return x """ def rej(a, b): """ Implements the rejection function for alternative diffusion. Args: a: Tensor of shape (B, H, W, C), where B is batch size, H and W are spatial dimensions, and C is number of channels. b: Tensor of the same shape as a. Returns: Tensor of the same shape as a and b, containing the rejection output. """ return (b * torch.tensordot(a, b, dims=len(a.shape)) / torch.tensordot(b, b, dims=len(a.shape))) - a @torch.no_grad() def sampler_euler_ancestral_dancing(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler=None, leap=2, eta_dance=1.0): #Ancestral sampling with Euler method steps, dancing steps. extra_args = {} if extra_args is None else extra_args noise_sampler = default_noise_sampler(x) if noise_sampler is None else noise_sampler unsample_noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) s_in = x.new_ones([x.shape[0]]) for i in trange(len(sigmas) - 1, disable=disable): if i < len(sigmas) - leap: is_danceable = sigmas[i + leap] > 0 else: is_danceable = False orig_x = x denoised = model(x, sigmas[i] * s_in, **extra_args) sigma_down, sigma_up = get_ancestral_step(sigmas[i], sigmas[i + leap] if is_danceable else sigmas[i + 1], eta=eta) if callback is not None: callback({'x': x, 'i': i, 'sigma': sigmas[i], 'sigma_hat': sigmas[i], 'denoised': denoised}) d = to_d(x, sigmas[i], denoised) # Euler method dt = sigma_down - sigmas[i] x = x + d * dt if sigmas[i + 1] > 0: if is_danceable: #x = x + noise_sampler(sigmas[i], sigmas[i + leap]) * s_noise * sigma_up #x = x + noise_sampler(sigmas[i + 2], sigmas[i + 1]) * s_noise * sigma_up denoised2 = model(x, sigmas[i + leap] * s_in, **extra_args) sigma_down2, sigma_up2 = get_ancestral_step(sigmas[i + leap], sigmas[i + 1], eta=eta_dance) d_2 = to_d(x, sigmas[i + leap], denoised2) dt_2 = sigma_down2 - sigmas[i + leap] x_2 = x + d_2 * dt_2 #x_2 = x_2 + noise_sampler(sigmas[i + leap], sigmas[i]) * s_noise * sigma_up2 sigma_down3, sigma_up3 = get_ancestral_step(sigmas[i], sigmas[i + 1], eta=eta) #x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * s_noise * sigma_up3 denoised3 = model(x_2, sigmas[i] * s_in, **extra_args) d_3 = to_d(orig_x, sigmas[i], denoised3 + rej(denoised3 - denoised, denoised2 - denoised)) #d_3 = to_d(x_2, sigmas[i], denoised3) dt_3 = sigma_down3 - sigmas[i] x = orig_x + d_3 * dt_3 # Very denoised, slightly denoised #print(dt_3, dt_2) x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * s_noise * sigma_up3 #x = x + d * dt else: x = x + noise_sampler(sigmas[i], sigmas[i + 1]) * s_noise * sigma_up return x def sample_euler_ancestral_dancing(model, x, sigmas, extra_args=None, callback=None, disable=None, eta=1., s_noise=1., noise_sampler="gaussian", leap=2, eta_dance=1.0): sigma_min, sigma_max = sigmas[sigmas > 0].min(), sigmas.max() seed = extra_args.get("seed", None) match noise_sampler: case "brownian": noise_sampler = BrownianTreeNoiseSampler(x, sigma_min, sigma_max, seed=seed, cpu=False) case "gaussian": noise_sampler = lambda sigma, sigma_next: torch.randn_like(x) case "uniform": noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 case "highres-pyramid": noise_sampler = lambda sigma, sigma_next: highres_pyramid_noise_like(x) case "perlin": noise_sampler = lambda sigma, sigma_next: rand_perlin_like(x) case "laplacian": noise_sampler = lambda sigma, sigma_next: rand_laplacian_like(x) case _: noise_sampler = lambda sigma, sigma_next: (torch.rand_like(x) - 0.5) * 2 * 1.73 return sampler_euler_ancestral_dancing(model, x, sigmas, extra_args=extra_args, callback=callback, disable=disable, eta=eta, s_noise=s_noise, noise_sampler=noise_sampler, leap=leap, eta_dance=eta_dance) # Add your personal samplers below here, just for formatting purposes ;3 # Add any extra samplers to the following dictionary extra_samplers = { "res_momentumized": sample_res_solver, "dpmpp_dualsde_momentumized": sample_dpmpp_dualsdemomentum, "clyb_4m_sde_momentumized": sample_clyb_4m_sde, "ttm": sample_ttmcustom, "lcm_custom_noise": sample_lcmcustom, "euler_ancestral_dancing": sample_euler_ancestral_dancing, } discard_penultimate_sigma_samplers = set(( "dpmpp_dualsde_momentumized", "clyb_4m_sde_momentumized" )) extra_schedulers = {}