/src/libjxl/lib/jxl/enc_photon_noise.cc
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1 | | // Copyright (c) the JPEG XL Project Authors. All rights reserved. |
2 | | // |
3 | | // Use of this source code is governed by a BSD-style |
4 | | // license that can be found in the LICENSE file. |
5 | | |
6 | | #include "lib/jxl/enc_photon_noise.h" |
7 | | |
8 | | #include <algorithm> |
9 | | #include <cmath> |
10 | | #include <cstddef> |
11 | | |
12 | | #include "lib/jxl/base/common.h" |
13 | | #include "lib/jxl/cms/opsin_params.h" |
14 | | #include "lib/jxl/noise.h" |
15 | | |
16 | | namespace jxl { |
17 | | |
18 | | namespace { |
19 | | |
20 | | // Assumes a daylight-like spectrum. |
21 | | // https://www.strollswithmydog.com/effective-quantum-efficiency-of-sensor/#:~:text=11%2C260%20photons/um%5E2/lx-s |
22 | | constexpr float kPhotonsPerLxSPerUm2 = 11260; |
23 | | |
24 | | // Order of magnitude for cameras in the 2010-2020 decade, taking the CFA into |
25 | | // account. |
26 | | constexpr float kEffectiveQuantumEfficiency = 0.20; |
27 | | |
28 | | // TODO(sboukortt): reevaluate whether these are good defaults, notably whether |
29 | | // it would be worth making read noise higher at lower ISO settings. |
30 | | constexpr float kPhotoResponseNonUniformity = 0.005; |
31 | | constexpr float kInputReferredReadNoise = 3; |
32 | | |
33 | | // Assumes a 35mm sensor. |
34 | | constexpr float kSensorAreaUm2 = 36000.f * 24000; |
35 | | |
36 | | template <typename T> |
37 | 0 | inline constexpr T Square(const T x) { |
38 | 0 | return x * x; |
39 | 0 | } |
40 | | template <typename T> |
41 | 0 | inline constexpr T Cube(const T x) { |
42 | 0 | return x * x * x; |
43 | 0 | } |
44 | | |
45 | | } // namespace |
46 | | |
47 | | NoiseParams SimulatePhotonNoise(const size_t xsize, const size_t ysize, |
48 | 0 | const float iso) { |
49 | 0 | const float kOpsinAbsorbanceBiasCbrt = |
50 | 0 | std::cbrt(jxl::cms::kOpsinAbsorbanceBias[1]); |
51 | | |
52 | | // Focal plane exposure for 18% of kDefaultIntensityTarget, in lx·s. |
53 | | // (ISO = 10 lx·s ÷ H) |
54 | 0 | const float h_18 = 10 / iso; |
55 | |
|
56 | 0 | const float pixel_area_um2 = kSensorAreaUm2 / (xsize * ysize); |
57 | |
|
58 | 0 | const float electrons_per_pixel_18 = kEffectiveQuantumEfficiency * |
59 | 0 | kPhotonsPerLxSPerUm2 * h_18 * |
60 | 0 | pixel_area_um2; |
61 | |
|
62 | 0 | NoiseParams params; |
63 | |
|
64 | 0 | for (size_t i = 0; i < NoiseParams::kNumNoisePoints; ++i) { |
65 | 0 | const float scaled_index = i / (NoiseParams::kNumNoisePoints - 2.f); |
66 | | // scaled_index is used for XYB = (0, 2·scaled_index, 2·scaled_index) |
67 | 0 | const float y = 2 * scaled_index; |
68 | | // 1 = default intensity target |
69 | 0 | const float linear = std::max(0.f, Cube(y - kOpsinAbsorbanceBiasCbrt) + |
70 | 0 | jxl::cms::kOpsinAbsorbanceBias[1]); |
71 | 0 | const float electrons_per_pixel = electrons_per_pixel_18 * (linear / 0.18f); |
72 | | // Quadrature sum of read noise, photon shot noise (sqrt(S) so simply not |
73 | | // squared here) and photo response non-uniformity. |
74 | | // https://doi.org/10.1117/3.725073 |
75 | | // Units are electrons rms. |
76 | 0 | const float noise = |
77 | 0 | std::sqrt(Square(kInputReferredReadNoise) + electrons_per_pixel + |
78 | 0 | Square(kPhotoResponseNonUniformity * electrons_per_pixel)); |
79 | 0 | const float linear_noise = noise * (0.18f / electrons_per_pixel_18); |
80 | 0 | const float opsin_derivative = |
81 | 0 | (1.f / 3) / |
82 | 0 | Square(std::cbrt(linear - jxl::cms::kOpsinAbsorbanceBias[1])); |
83 | 0 | const float opsin_noise = linear_noise * opsin_derivative; |
84 | | |
85 | | // TODO(sboukortt): verify more thoroughly whether the denominator is |
86 | | // correct. |
87 | 0 | params.lut[i] = |
88 | 0 | Clamp1(opsin_noise / |
89 | 0 | (0.22f // norm_const |
90 | 0 | * std::sqrt(2.f) // red_noise + green_noise |
91 | 0 | * 1.13f // standard deviation of a plane of generated noise |
92 | 0 | ), |
93 | 0 | 0.f, 1.f); |
94 | 0 | } |
95 | |
|
96 | 0 | return params; |
97 | 0 | } |
98 | | |
99 | | } // namespace jxl |