583f2bdd13
BOMs barf on UTF-8 decoding within PyTorch: File "D:\Soft\Miniconda3\lib\site-packages\torch\utils_cpp_extension_versioner.py", line 16, in hash_source_files hash_value = update_hash(hash_value, file.read()) UnicodeDecodeError: 'gbk' codec can't decode byte 0xbf in position 2: illegal multibyte sequence Should fix #10, #14
267 lines
11 KiB
Python
267 lines
11 KiB
Python
# Copyright (c) 2021, NVIDIA CORPORATION & AFFILIATES. All rights reserved.
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#
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# NVIDIA CORPORATION and its licensors retain all intellectual property
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# and proprietary rights in and to this software, related documentation
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# and any modifications thereto. Any use, reproduction, disclosure or
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# distribution of this software and related documentation without an express
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# license agreement from NVIDIA CORPORATION is strictly prohibited.
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"""Equivariance metrics (EQ-T, EQ-T_frac, and EQ-R) from the paper
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"Alias-Free Generative Adversarial Networks"."""
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import copy
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import numpy as np
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import torch
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import torch.fft
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from torch_utils.ops import upfirdn2d
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from . import metric_utils
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#----------------------------------------------------------------------------
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# Utilities.
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def sinc(x):
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y = (x * np.pi).abs()
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z = torch.sin(y) / y.clamp(1e-30, float('inf'))
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return torch.where(y < 1e-30, torch.ones_like(x), z)
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def lanczos_window(x, a):
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x = x.abs() / a
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return torch.where(x < 1, sinc(x), torch.zeros_like(x))
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def rotation_matrix(angle):
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angle = torch.as_tensor(angle).to(torch.float32)
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mat = torch.eye(3, device=angle.device)
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mat[0, 0] = angle.cos()
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mat[0, 1] = angle.sin()
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mat[1, 0] = -angle.sin()
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mat[1, 1] = angle.cos()
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return mat
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#----------------------------------------------------------------------------
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# Apply integer translation to a batch of 2D images. Corresponds to the
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# operator T_x in Appendix E.1.
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def apply_integer_translation(x, tx, ty):
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_N, _C, H, W = x.shape
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tx = torch.as_tensor(tx * W).to(dtype=torch.float32, device=x.device)
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ty = torch.as_tensor(ty * H).to(dtype=torch.float32, device=x.device)
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ix = tx.round().to(torch.int64)
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iy = ty.round().to(torch.int64)
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z = torch.zeros_like(x)
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m = torch.zeros_like(x)
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if abs(ix) < W and abs(iy) < H:
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y = x[:, :, max(-iy,0) : H+min(-iy,0), max(-ix,0) : W+min(-ix,0)]
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z[:, :, max(iy,0) : H+min(iy,0), max(ix,0) : W+min(ix,0)] = y
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m[:, :, max(iy,0) : H+min(iy,0), max(ix,0) : W+min(ix,0)] = 1
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return z, m
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#----------------------------------------------------------------------------
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# Apply integer translation to a batch of 2D images. Corresponds to the
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# operator T_x in Appendix E.2.
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def apply_fractional_translation(x, tx, ty, a=3):
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_N, _C, H, W = x.shape
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tx = torch.as_tensor(tx * W).to(dtype=torch.float32, device=x.device)
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ty = torch.as_tensor(ty * H).to(dtype=torch.float32, device=x.device)
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ix = tx.floor().to(torch.int64)
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iy = ty.floor().to(torch.int64)
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fx = tx - ix
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fy = ty - iy
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b = a - 1
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z = torch.zeros_like(x)
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zx0 = max(ix - b, 0)
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zy0 = max(iy - b, 0)
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zx1 = min(ix + a, 0) + W
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zy1 = min(iy + a, 0) + H
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if zx0 < zx1 and zy0 < zy1:
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taps = torch.arange(a * 2, device=x.device) - b
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filter_x = (sinc(taps - fx) * sinc((taps - fx) / a)).unsqueeze(0)
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filter_y = (sinc(taps - fy) * sinc((taps - fy) / a)).unsqueeze(1)
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y = x
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y = upfirdn2d.filter2d(y, filter_x / filter_x.sum(), padding=[b,a,0,0])
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y = upfirdn2d.filter2d(y, filter_y / filter_y.sum(), padding=[0,0,b,a])
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y = y[:, :, max(b-iy,0) : H+b+a+min(-iy-a,0), max(b-ix,0) : W+b+a+min(-ix-a,0)]
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z[:, :, zy0:zy1, zx0:zx1] = y
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m = torch.zeros_like(x)
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mx0 = max(ix + a, 0)
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my0 = max(iy + a, 0)
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mx1 = min(ix - b, 0) + W
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my1 = min(iy - b, 0) + H
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if mx0 < mx1 and my0 < my1:
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m[:, :, my0:my1, mx0:mx1] = 1
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return z, m
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#----------------------------------------------------------------------------
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# Construct an oriented low-pass filter that applies the appropriate
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# bandlimit with respect to the input and output of the given affine 2D
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# image transformation.
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def construct_affine_bandlimit_filter(mat, a=3, amax=16, aflt=64, up=4, cutoff_in=1, cutoff_out=1):
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assert a <= amax < aflt
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mat = torch.as_tensor(mat).to(torch.float32)
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# Construct 2D filter taps in input & output coordinate spaces.
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taps = ((torch.arange(aflt * up * 2 - 1, device=mat.device) + 1) / up - aflt).roll(1 - aflt * up)
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yi, xi = torch.meshgrid(taps, taps)
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xo, yo = (torch.stack([xi, yi], dim=2) @ mat[:2, :2].t()).unbind(2)
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# Convolution of two oriented 2D sinc filters.
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fi = sinc(xi * cutoff_in) * sinc(yi * cutoff_in)
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fo = sinc(xo * cutoff_out) * sinc(yo * cutoff_out)
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f = torch.fft.ifftn(torch.fft.fftn(fi) * torch.fft.fftn(fo)).real
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# Convolution of two oriented 2D Lanczos windows.
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wi = lanczos_window(xi, a) * lanczos_window(yi, a)
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wo = lanczos_window(xo, a) * lanczos_window(yo, a)
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w = torch.fft.ifftn(torch.fft.fftn(wi) * torch.fft.fftn(wo)).real
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# Construct windowed FIR filter.
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f = f * w
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# Finalize.
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c = (aflt - amax) * up
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f = f.roll([aflt * up - 1] * 2, dims=[0,1])[c:-c, c:-c]
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f = torch.nn.functional.pad(f, [0, 1, 0, 1]).reshape(amax * 2, up, amax * 2, up)
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f = f / f.sum([0,2], keepdim=True) / (up ** 2)
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f = f.reshape(amax * 2 * up, amax * 2 * up)[:-1, :-1]
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return f
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#----------------------------------------------------------------------------
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# Apply the given affine transformation to a batch of 2D images.
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def apply_affine_transformation(x, mat, up=4, **filter_kwargs):
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_N, _C, H, W = x.shape
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mat = torch.as_tensor(mat).to(dtype=torch.float32, device=x.device)
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# Construct filter.
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f = construct_affine_bandlimit_filter(mat, up=up, **filter_kwargs)
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assert f.ndim == 2 and f.shape[0] == f.shape[1] and f.shape[0] % 2 == 1
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p = f.shape[0] // 2
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# Construct sampling grid.
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theta = mat.inverse()
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theta[:2, 2] *= 2
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theta[0, 2] += 1 / up / W
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theta[1, 2] += 1 / up / H
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theta[0, :] *= W / (W + p / up * 2)
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theta[1, :] *= H / (H + p / up * 2)
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theta = theta[:2, :3].unsqueeze(0).repeat([x.shape[0], 1, 1])
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g = torch.nn.functional.affine_grid(theta, x.shape, align_corners=False)
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# Resample image.
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y = upfirdn2d.upsample2d(x=x, f=f, up=up, padding=p)
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z = torch.nn.functional.grid_sample(y, g, mode='bilinear', padding_mode='zeros', align_corners=False)
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# Form mask.
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m = torch.zeros_like(y)
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c = p * 2 + 1
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m[:, :, c:-c, c:-c] = 1
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m = torch.nn.functional.grid_sample(m, g, mode='nearest', padding_mode='zeros', align_corners=False)
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return z, m
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#----------------------------------------------------------------------------
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# Apply fractional rotation to a batch of 2D images. Corresponds to the
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# operator R_\alpha in Appendix E.3.
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def apply_fractional_rotation(x, angle, a=3, **filter_kwargs):
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angle = torch.as_tensor(angle).to(dtype=torch.float32, device=x.device)
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mat = rotation_matrix(angle)
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return apply_affine_transformation(x, mat, a=a, amax=a*2, **filter_kwargs)
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#----------------------------------------------------------------------------
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# Modify the frequency content of a batch of 2D images as if they had undergo
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# fractional rotation -- but without actually rotating them. Corresponds to
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# the operator R^*_\alpha in Appendix E.3.
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def apply_fractional_pseudo_rotation(x, angle, a=3, **filter_kwargs):
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angle = torch.as_tensor(angle).to(dtype=torch.float32, device=x.device)
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mat = rotation_matrix(-angle)
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f = construct_affine_bandlimit_filter(mat, a=a, amax=a*2, up=1, **filter_kwargs)
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y = upfirdn2d.filter2d(x=x, f=f)
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m = torch.zeros_like(y)
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c = f.shape[0] // 2
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m[:, :, c:-c, c:-c] = 1
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return y, m
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#----------------------------------------------------------------------------
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# Compute the selected equivariance metrics for the given generator.
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def compute_equivariance_metrics(opts, num_samples, batch_size, translate_max=0.125, rotate_max=1, compute_eqt_int=False, compute_eqt_frac=False, compute_eqr=False):
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assert compute_eqt_int or compute_eqt_frac or compute_eqr
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# Setup generator and labels.
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G = copy.deepcopy(opts.G).eval().requires_grad_(False).to(opts.device)
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I = torch.eye(3, device=opts.device)
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M = getattr(getattr(getattr(G, 'synthesis', None), 'input', None), 'transform', None)
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if M is None:
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raise ValueError('Cannot compute equivariance metrics; the given generator does not support user-specified image transformations')
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c_iter = metric_utils.iterate_random_labels(opts=opts, batch_size=batch_size)
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# Sampling loop.
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sums = None
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progress = opts.progress.sub(tag='eq sampling', num_items=num_samples)
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for batch_start in range(0, num_samples, batch_size * opts.num_gpus):
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progress.update(batch_start)
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s = []
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# Randomize noise buffers, if any.
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for name, buf in G.named_buffers():
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if name.endswith('.noise_const'):
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buf.copy_(torch.randn_like(buf))
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# Run mapping network.
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z = torch.randn([batch_size, G.z_dim], device=opts.device)
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c = next(c_iter)
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ws = G.mapping(z=z, c=c)
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# Generate reference image.
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M[:] = I
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orig = G.synthesis(ws=ws, noise_mode='const', **opts.G_kwargs)
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# Integer translation (EQ-T).
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if compute_eqt_int:
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t = (torch.rand(2, device=opts.device) * 2 - 1) * translate_max
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t = (t * G.img_resolution).round() / G.img_resolution
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M[:] = I
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M[:2, 2] = -t
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img = G.synthesis(ws=ws, noise_mode='const', **opts.G_kwargs)
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ref, mask = apply_integer_translation(orig, t[0], t[1])
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s += [(ref - img).square() * mask, mask]
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# Fractional translation (EQ-T_frac).
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if compute_eqt_frac:
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t = (torch.rand(2, device=opts.device) * 2 - 1) * translate_max
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M[:] = I
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M[:2, 2] = -t
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img = G.synthesis(ws=ws, noise_mode='const', **opts.G_kwargs)
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ref, mask = apply_fractional_translation(orig, t[0], t[1])
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s += [(ref - img).square() * mask, mask]
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# Rotation (EQ-R).
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if compute_eqr:
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angle = (torch.rand([], device=opts.device) * 2 - 1) * (rotate_max * np.pi)
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M[:] = rotation_matrix(-angle)
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img = G.synthesis(ws=ws, noise_mode='const', **opts.G_kwargs)
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ref, ref_mask = apply_fractional_rotation(orig, angle)
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pseudo, pseudo_mask = apply_fractional_pseudo_rotation(img, angle)
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mask = ref_mask * pseudo_mask
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s += [(ref - pseudo).square() * mask, mask]
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# Accumulate results.
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s = torch.stack([x.to(torch.float64).sum() for x in s])
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sums = sums + s if sums is not None else s
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progress.update(num_samples)
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# Compute PSNRs.
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if opts.num_gpus > 1:
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torch.distributed.all_reduce(sums)
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sums = sums.cpu()
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mses = sums[0::2] / sums[1::2]
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psnrs = np.log10(2) * 20 - mses.log10() * 10
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psnrs = tuple(psnrs.numpy())
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return psnrs[0] if len(psnrs) == 1 else psnrs
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#----------------------------------------------------------------------------
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