Datasets:
filename stringlengths 28 96 | decomp_family stringclasses 25
values | decomp_params stringclasses 534
values | upsamp_method stringclasses 19
values | upsamp_params stringclasses 20
values | scale int32 2 16 | category stringclasses 6
values | signature list | umap_2d list | umap_3d list | image imagewidth (px) 256 256 |
|---|---|---|---|---|---|---|---|---|---|---|
anisotropic_diffusion_gamma0.05_iterations10_kappa100___area_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | area | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___area_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | area | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___area_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | area | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bicubic_16x_scale16.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bicubic_16x | {"scale": 16} | 16 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bicubic_3x_scale3.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bicubic_3x | {"scale": 3} | 3 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bicubic_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bicubic | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bicubic_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bicubic | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bicubic_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bicubic | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bilinear_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bilinear | {"scale": 2} | 2 | edge_preserving | [
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0.0335000120103... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bilinear_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bilinear | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bilinear_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bilinear | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bspline_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bspline | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bspline_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bspline | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___bspline_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | bspline | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___cubic_catmull_rom_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | cubic_catmull_rom | {"scale": 2} | 2 | edge_preserving | [
0.04095974564552307,
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0.0328182540833... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___cubic_catmull_rom_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | cubic_catmull_rom | {"scale": 4} | 4 | edge_preserving | [
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0.032649818807840... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___cubic_catmull_rom_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | cubic_catmull_rom | {"scale": 8} | 8 | edge_preserving | [
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0.03260838612914085... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___cubic_mitchell_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | cubic_mitchell | {"scale": 2} | 2 | edge_preserving | [
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0.033447146415... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___cubic_mitchell_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | cubic_mitchell | {"scale": 4} | 4 | edge_preserving | [
0.041813068091869354,
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0.033358182758... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___cubic_mitchell_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | cubic_mitchell | {"scale": 8} | 8 | edge_preserving | [
0.04171419143676758,
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0.033316310495... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___edge_directed_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | edge_directed | {"scale": 2} | 2 | edge_preserving | [
0.0409625805914402,
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0.03281714394... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___edge_directed_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | edge_directed | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___fft_zeropad_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | fft_zeropad | {"scale": 2} | 2 | edge_preserving | [
0.04194207489490509,
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0.032520297914743... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___fft_zeropad_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | fft_zeropad | {"scale": 4} | 4 | edge_preserving | [
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0.0324165560305... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___fft_zeropad_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | fft_zeropad | {"scale": 8} | 8 | edge_preserving | [
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0.03241014480590... | [
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa100___lanczos_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | lanczos | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___lanczos_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | lanczos | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___lanczos_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | lanczos | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___linear_exact_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | linear_exact | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___linear_exact_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | linear_exact | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___linear_exact_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | linear_exact | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___nearest_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | nearest | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___nearest_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | nearest | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___nearest_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | nearest | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quadratic_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quadratic | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quadratic_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quadratic | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quadratic_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quadratic | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quartic_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quartic | {"scale": 2} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quartic_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quartic | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quartic_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quartic | {"scale": 8} | 8 | edge_preserving | [
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0.03253084793686... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quintic_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quintic | {"scale": 2} | 2 | edge_preserving | [
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0.03269717469... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quintic_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quintic | {"scale": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___quintic_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | quintic | {"scale": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___regularized_lambda_reg0.001_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | regularized | {"scale": 2, "lambda_reg": 0.001} | 2 | edge_preserving | [
0.040949009358882904,
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0.032776340... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___regularized_lambda_reg0.001_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | regularized | {"scale": 4, "lambda_reg": 0.001} | 4 | edge_preserving | [
0.04048067703843117,
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa100___regularized_lambda_reg0.01_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | regularized | {"scale": 2, "lambda_reg": 0.01} | 2 | edge_preserving | [
0.04052207991480827,
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___regularized_lambda_reg0.01_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | regularized | {"scale": 4, "lambda_reg": 0.01} | 4 | edge_preserving | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___regularized_lambda_reg0.1_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | regularized | {"scale": 2, "lambda_reg": 0.1} | 2 | edge_preserving | [
0.034019835293293,
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0.0316362939774... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___regularized_lambda_reg0.1_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | regularized | {"scale": 4, "lambda_reg": 0.1} | 4 | edge_preserving | [
0.03732796758413315,
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size16_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 2, "kernel_size": 16} | 2 | edge_preserving | [
0.04072696343064308,
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0.0327324829... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size16_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 4, "kernel_size": 16} | 4 | edge_preserving | [
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0.03278907015919685... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size16_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 8, "kernel_size": 16} | 8 | edge_preserving | [
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0.033075299113988... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size4_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 2, "kernel_size": 4} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size4_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 4, "kernel_size": 4} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size4_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 8, "kernel_size": 4} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size8_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 2, "kernel_size": 8} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size8_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 4, "kernel_size": 8} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_blackman_kernel_size8_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_blackman | {"scale": 8, "kernel_size": 8} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size16_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 2, "kernel_size": 16} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size16_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 4, "kernel_size": 16} | 4 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size16_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 8, "kernel_size": 16} | 8 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size4_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 2, "kernel_size": 4} | 2 | edge_preserving | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size4_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 4, "kernel_size": 4} | 4 | edge_preserving | [
0.04077305272221565,
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0.0329522490501... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size4_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 8, "kernel_size": 4} | 8 | edge_preserving | [
0.03722504526376724,
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size8_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 2, "kernel_size": 8} | 2 | edge_preserving | [
0.04075230658054352,
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size8_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 4, "kernel_size": 8} | 4 | edge_preserving | [
0.0407317616045475,
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0.0330605879426... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa100___sinc_hamming_kernel_size8_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 100, "gamma": 0.05} | sinc_hamming | {"scale": 8, "kernel_size": 8} | 8 | edge_preserving | [
0.04071587696671486,
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0.0329610444... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___area_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | area | {"scale": 2} | 2 | edge_preserving | [
0.04094114527106285,
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___area_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | area | {"scale": 4} | 4 | edge_preserving | [
0.04012971743941307,
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___area_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | area | {"scale": 8} | 8 | edge_preserving | [
0.0402287021279335,
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___bicubic_16x_scale16.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bicubic_16x | {"scale": 16} | 16 | edge_preserving | [
0.04048176854848862,
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___bicubic_3x_scale3.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bicubic_3x | {"scale": 3} | 3 | edge_preserving | [
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0.032660175114870... | [
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] | [
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___bicubic_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bicubic | {"scale": 2} | 2 | edge_preserving | [
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0.0327889323234... | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___bicubic_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bicubic | {"scale": 4} | 4 | edge_preserving | [
0.0405999980866909,
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0.0326161384582... | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___bicubic_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bicubic | {"scale": 8} | 8 | edge_preserving | [
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] | [
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anisotropic_diffusion_gamma0.05_iterations10_kappa10___bilinear_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bilinear | {"scale": 2} | 2 | edge_preserving | [
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0.03347408398985863... | [
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] | [
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___bilinear_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bilinear | {"scale": 4} | 4 | edge_preserving | [
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0.0331783369183... | [
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] | [
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___bilinear_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bilinear | {"scale": 8} | 8 | edge_preserving | [
0.04224959388375282,
0.037388768047094345,
0.03737102076411247,
0.03745623677968979,
0.03734708949923515,
0.03670629858970642,
0.03624626249074936,
0.03661959245800972,
0.03600877523422241,
0.03583807870745659,
0.034748706966638565,
0.03407088294625282,
0.0336473248898983,
0.03308662772178... | [
-3.377607583999634,
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] | [
-1.6575615406036377,
1.025903344154358,
6.2367706298828125
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___bspline_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bspline | {"scale": 2} | 2 | edge_preserving | [
0.04111147299408913,
0.03655189275741577,
0.03620537370443344,
0.03646072372794151,
0.036367520689964294,
0.035853445529937744,
0.03531023859977722,
0.0358082540333271,
0.03510119765996933,
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0.034213144332170486,
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0.03326469659805298,
0.032840292900... | [
3.1290552616119385,
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] | [
-3.8217124938964844,
0.6242838501930237,
5.2920942306518555
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___bspline_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bspline | {"scale": 4} | 4 | edge_preserving | [
0.040687303990125656,
0.03619754686951637,
0.03587459772825241,
0.03612098842859268,
0.036062419414520264,
0.03549530357122421,
0.035024408251047134,
0.03552640601992607,
0.0349234938621521,
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0.03265329822... | [
3.9560816287994385,
-6.5092597007751465
] | [
-4.57323694229126,
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4.805410861968994
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___bspline_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | bspline | {"scale": 8} | 8 | edge_preserving | [
0.04057638347148895,
0.03609698638319969,
0.03578390181064606,
0.03602750971913338,
0.035973697900772095,
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0.03260396048426... | [
4.266958236694336,
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] | [
-4.783716201782227,
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4.644712448120117
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___cubic_catmull_rom_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | cubic_catmull_rom | {"scale": 2} | 2 | edge_preserving | [
0.04104074090719223,
0.03651557117700577,
0.03611643984913826,
0.03639880195260048,
0.03633773699402809,
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0.03524857386946678,
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0.0327889323234... | [
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] | [
-3.840317964553833,
0.5936269164085388,
5.296286582946777
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___cubic_catmull_rom_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | cubic_catmull_rom | {"scale": 4} | 4 | edge_preserving | [
0.0405999980866909,
0.036160122603178024,
0.035766761749982834,
0.036065127700567245,
0.03601064160466194,
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0.0326161384582... | [
4.2752838134765625,
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] | [
-4.762633323669434,
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4.657781600952148
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___cubic_catmull_rom_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | cubic_catmull_rom | {"scale": 8} | 8 | edge_preserving | [
0.04050539433956146,
0.03606313839554787,
0.03567279875278473,
0.03598257154226303,
0.03592513129115105,
0.035312242805957794,
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0.0325713939... | [
4.46240234375,
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] | [
-4.8629279136657715,
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4.498269557952881
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___cubic_mitchell_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | cubic_mitchell | {"scale": 2} | 2 | edge_preserving | [
0.042376838624477386,
0.037783149629831314,
0.03733592852950096,
0.03756200149655342,
0.03753601387143135,
0.037049319595098495,
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0.0348711758852005,
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0.0334335267543... | [
-3.3706533908843994,
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] | [
-1.3467439413070679,
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___cubic_mitchell_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | cubic_mitchell | {"scale": 4} | 4 | edge_preserving | [
0.04192481189966202,
0.03745793551206589,
0.03696584701538086,
0.03726128861308098,
0.037240371108055115,
0.03672044351696968,
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0.03403078392148018,
0.03379804268479347,
0.03332317247... | [
-3.392503499984741,
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] | [
-1.8633838891983032,
0.9770821928977966,
6.286676406860352
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___cubic_mitchell_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | cubic_mitchell | {"scale": 8} | 8 | edge_preserving | [
0.04182439297437668,
0.03737170994281769,
0.03683776408433914,
0.03716475889086723,
0.0371464341878891,
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0.03599504008889198,
0.03650153428316116,
0.03569987788796425,
0.0357673205435276,
0.03447674959897995,
0.033953770995140076,
0.03378809243440628,
0.033277627080678... | [
-3.3347198963165283,
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] | [
-1.9164364337921143,
1.0020641088485718,
6.2416090965271
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___edge_directed_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | edge_directed | {"scale": 2} | 2 | edge_preserving | [
0.04104890674352646,
0.03651416674256325,
0.03610709682106972,
0.03639032319188118,
0.03632813319563866,
0.03578881174325943,
0.035245757550001144,
0.03576933220028877,
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0.034147556871175766,
0.033553652465343475,
0.033241912722587585,
0.03278454765... | [
3.2322771549224854,
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] | [
-3.8984172344207764,
0.5389402508735657,
5.262850284576416
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___edge_directed_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | edge_directed | {"scale": 4} | 4 | edge_preserving | [
0.04062622785568237,
0.03616272285580635,
0.035757847130298615,
0.03605494648218155,
0.03601080924272537,
0.03541158139705658,
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0.0326169431209... | [
4.246482849121094,
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] | [
-4.769474506378174,
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4.641617298126221
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___fft_zeropad_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | fft_zeropad | {"scale": 2} | 2 | edge_preserving | [
0.040681835263967514,
0.03621787205338478,
0.03581904247403145,
0.03600963577628136,
0.03602461516857147,
0.035611532628536224,
0.03501005843281746,
0.035519056022167206,
0.034826770424842834,
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0.033803392201662064,
0.03321949765086174,
0.033003125339746475,
0.032587617... | [
4.519300937652588,
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] | [
-4.78575325012207,
-0.6764153242111206,
4.414828300476074
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___fft_zeropad_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | fft_zeropad | {"scale": 4} | 4 | edge_preserving | [
0.04024277627468109,
0.03587115928530693,
0.03546910732984543,
0.035697415471076965,
0.03573020547628403,
0.03524896502494812,
0.03469794988632202,
0.03520257771015167,
0.03449204936623573,
0.03463122993707657,
0.033467847853899,
0.0329551137983799,
0.03283270075917244,
0.03246060386300087... | [
5.015092372894287,
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] | [
-4.366049289703369,
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3.697118043899536
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___fft_zeropad_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | fft_zeropad | {"scale": 8} | 8 | edge_preserving | [
0.04017746075987816,
0.03578348830342293,
0.035363372415304184,
0.035606082528829575,
0.0356520377099514,
0.035166990011930466,
0.03461608290672302,
0.03511043265461922,
0.034422121942043304,
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0.032912176102399826,
0.032806821167469025,
0.0324187576... | [
5.06041145324707,
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] | [
-4.353126525878906,
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___lanczos_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | lanczos | {"scale": 2} | 2 | edge_preserving | [
0.040876604616642,
0.036381796002388,
0.03598012775182724,
0.03624789044260979,
0.03620869666337967,
0.03567884489893913,
0.03512665256857872,
0.03567185625433922,
0.03492065146565437,
0.034988388419151306,
0.033956315368413925,
0.03334847837686539,
0.0330888070166111,
0.032641712576150894... | [
3.878596782684326,
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] | [
-4.456079006195068,
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4.855218887329102
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___lanczos_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | lanczos | {"scale": 4} | 4 | edge_preserving | [
0.04044806957244873,
0.03603145107626915,
0.0356254018843174,
0.03591185435652733,
0.03586583584547043,
0.035333577543497086,
0.03482971712946892,
0.03537054732441902,
0.034644123166799545,
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0.0336281880736351,
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0.032501012086868... | [
4.6403584480285645,
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] | [
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___lanczos_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | lanczos | {"scale": 8} | 8 | edge_preserving | [
0.04035288468003273,
0.03593834489583969,
0.035533662885427475,
0.0358247272670269,
0.035777587443590164,
0.035246603190898895,
0.0347411222755909,
0.03527538850903511,
0.034566041082143784,
0.03468924015760422,
0.03354751691222191,
0.03307536989450455,
0.032882191240787506,
0.032449185848... | [
4.710292816162109,
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] | [
-4.837964057922363,
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___linear_exact_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | linear_exact | {"scale": 2} | 2 | edge_preserving | [
0.04314395412802696,
0.038343727588653564,
0.03802836313843727,
0.038195934146642685,
0.03808288648724556,
0.037487369030714035,
0.036886654794216156,
0.03733782842755318,
0.036499474197626114,
0.0365099161863327,
0.035299401730298996,
0.03453144058585167,
0.03410595655441284,
0.0335639268... | [
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] | [
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___linear_exact_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | linear_exact | {"scale": 4} | 4 | edge_preserving | [
0.04229027032852173,
0.037619516253471375,
0.03752414509654045,
0.03758269175887108,
0.037584107369184494,
0.036889396607875824,
0.03634173795580864,
0.03677459433674812,
0.03605322912335396,
0.03610073775053024,
0.03480536863207817,
0.03417492285370827,
0.03372962400317192,
0.033240221440... | [
-3.372544765472412,
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] | [
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1.0186877250671387,
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___linear_exact_scale8.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | linear_exact | {"scale": 8} | 8 | edge_preserving | [
0.04210915416479111,
0.03741062432527542,
0.037400227040052414,
0.03742978721857071,
0.03750564157962799,
0.036753468215465546,
0.03617853298783302,
0.03660313040018082,
0.0359133742749691,
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0.03361839801073074,
0.0331271216273... | [
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] | [
-1.652653694152832,
1.025566816329956,
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] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___nearest_scale2.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | nearest | {"scale": 2} | 2 | edge_preserving | [
0.04094114527106285,
0.03603459149599075,
0.03675619885325432,
0.03638632595539093,
0.03668805584311485,
0.03582269325852394,
0.03544960170984268,
0.03585164248943329,
0.03530549630522728,
0.03521666303277016,
0.034181345254182816,
0.03350682556629181,
0.03317287191748619,
0.03269548341631... | [
3.43268084526062,
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] | [
-4.006128787994385,
0.6608526110649109,
5.154544830322266
] | |
anisotropic_diffusion_gamma0.05_iterations10_kappa10___nearest_scale4.npy | anisotropic_diffusion | {"iterations": 10, "kappa": 10, "gamma": 0.05} | nearest | {"scale": 4} | 4 | edge_preserving | [
0.04052403196692467,
0.036020226776599884,
0.036550868302583694,
0.03590701147913933,
0.03616821765899658,
0.035509414970874786,
0.03522258624434471,
0.03549811989068985,
0.03524691238999367,
0.03492862731218338,
0.03381722420454025,
0.03335651755332947,
0.03293284401297569,
0.032284118235... | [
4.33034610748291,
-6.736067771911621
] | [
-4.805079460144043,
-0.392401784658432,
4.594437122344971
] |
RESIDUALS — LiDAR DEM residual fingerprints
39,716 residual images extracted by applying 593 distinct decomposition configurations × 25 upsampling methods to a single Fairfield County, Ohio LiDAR-derived Digital Elevation Model (1500×375 at 3.33 ft/px). Each row pairs a 256×256 PNG of the residual (rendered with the standard RdBu_r colormap, 99th-percentile symmetric clipping) with the algorithm and parameters that produced it, plus a 40-dim signature vector and pre-computed 2D/3D UMAP coordinates.
The companion source-code project is RESIDUALS; the rendered atlas / sweep videos / Blender flythrough that visualize this dataset are produced by the residuals-visuals project.
Why this dataset is interesting
- Algorithm classification benchmark: predict which decomposition algorithm produced a residual (24 family classes, or 593 fine-grained classes). A non-trivial visual task — many algorithm families produce visually similar outputs at certain parameter settings.
- Algorithm fingerprinting / signal-processing forensics: the included 40-dim signatures (radial-FFT power spectrum + statistical moments) cluster algorithm families clearly in UMAP space — useful as a reference for inverse-problem and provenance work.
- Same scene, all algorithms: every residual is a different mathematical lens on the same underlying terrain, making this an unusually clean substrate for studying what each algorithm preserves vs. destroys.
- Reproducible: source DEM hashes + RESIDUALS source code = full regeneration of the original 4.28 TB float64 outputs.
Schema
| Column | Type | Description |
|---|---|---|
filename |
string | Original .npy filename in the source RESIDUALS exhaustive run |
decomp_family |
string | e.g. gaussian, wavelet_biorthogonal, morphological_rect, anisotropic_diffusion |
decomp_params |
string (JSON) | e.g. {"sigma": 10} or {"wavelet": "bior3.5", "level": 3} |
upsamp_method |
string | e.g. bicubic, lanczos, fft_zeropad, sinc_hamming |
upsamp_params |
string (JSON) | e.g. {"scale": 2, "kernel_size": 8} |
scale |
int32 | Upsampling factor: 2, 3, 4, 8, or 16 |
category |
string | Meta-category: classical, edge_preserving, wavelet, morphological, trend_removal, multiscale |
signature |
list[40] | 32-bin radial-FFT log-power spectrum + 8 statistical moments (mean, std, skew, kurtosis, p50|abs|, p99|abs|, edge density, lag-1 autocorrelation) |
umap_2d |
list[2] | 2D UMAP embedding of the signature |
umap_3d |
list[3] | 3D UMAP embedding of the signature |
image |
binary (PNG) | 256×256 PNG of the residual, RdBu_r colormap, 99th-pctile symmetric clip |
Source data
- DEM: 1500×375 array, 3.33 ft/px resolution, derived from LiDAR tiles
BS000600.lasthroughBS000603.lascovering ~1 mi² in Fairfield County, Ohio. Z range: 808.5–1034.4 ft. CRS: Ohio State Plane South (EPSG:3735). - Residual crop: 640×640 region at scale=2 coordinates
(row=1600, col=400), normalized to 256×256. Region was selected for high feature density (sweeping diagonal stream channel, branching drainage, V-shaped linear feature, distinct ridge/embankment patterns). - 15 of the original 39,731 files are excluded due to division-by-zero edge cases in signature computation (all
bicubic_16x_scale=16outputs).
Splits
Single train split with 39,716 rows. The dataset is small enough that downstream users typically define their own splits (e.g. by decomp_family for held-out generalization, or random for IID evaluation).
Quick start
from datasets import load_dataset
ds = load_dataset("bshepp/residuals-fingerprints")
print(ds)
print(ds["train"][0]["decomp_family"], ds["train"][0]["decomp_params"])
ds["train"][0]["image"] # PIL.Image.Image, 256x256
Citation
The canonical citation is the Zenodo archive (which contains the full data + visualizations + code snapshot):
@dataset{sheppard_residuals_2026,
author = {Sheppard, Brian},
title = {RESIDUALS: 39,731-residual exhaustive parameter sweep of
decomposition × upsampling methods on a Fairfield County,
Ohio LiDAR DEM},
year = 2026,
publisher = {Zenodo},
doi = {10.5281/zenodo.19903273},
url = {https://doi.org/10.5281/zenodo.19903273}
}
Or this Hugging Face dataset (rendered subset for ML use):
@dataset{sheppard_residuals_fingerprints_2026,
author = {Sheppard, Brian},
title = {RESIDUALS — LiDAR DEM residual fingerprints (39,716 rows)},
year = 2026,
publisher = {Hugging Face},
url = {https://huggingface.co/datasets/bshepp/residuals-fingerprints}
}
Project page: https://residuals.briansheppard.com · Source code: https://github.com/bshepp/residuals-visuals · Source pipeline: https://github.com/bshepp/RESIDUALS
License
Apache 2.0 — same as the source RESIDUALS project.
Limitations and ethics
- Single scene: all 39,716 samples come from the same DEM. Models trained here may not generalize to other terrains. Treat as a fingerprinting benchmark, not a generic remote-sensing pretraining set.
- Class imbalance: family counts range from 201 (
polynomial) to 5,346 (wavelet). Use stratified splits or balanced sampling if classification accuracy matters. - Known artifact: the leftmost ~30 columns of the source DEM exhibit upsampling-boundary effects. The crop window dodges this entirely.
- No PII / sensitive content: terrain residuals only. The source LiDAR is publicly-available Ohio state data.
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