|
| 1 | +""" |
| 2 | +Title: Fresnel Diffraction for Coherent and Monochromatic |
| 3 | + Wave Fields |
| 4 | +
|
| 5 | +Fresnel Diffraction describes the behavior of a wave field as it |
| 6 | +moves through free space or interacts with an object under the |
| 7 | +small-angle approximation. It is particularly useful for near |
| 8 | +field diffraction. |
| 9 | +
|
| 10 | +The following algorithm is an adaptation of the 'transfer function' |
| 11 | +based approach contained in the reference. It is critically |
| 12 | +sampled when: |
| 13 | +pixel_size = wavelength * prop_dist / side_length |
| 14 | +
|
| 15 | +Or equivalently: |
| 16 | +pixel_size = sqrt(wavelength * prop_dist / pixel_num) |
| 17 | +
|
| 18 | +Under and oversampling occur when the left-hand side is less |
| 19 | +than or greater than the right-hand side, respectively. |
| 20 | +
|
| 21 | +This code is adapted and modified from: |
| 22 | +Computational Fourier Optics: A MATLAB Tutorial by David Voelz |
| 23 | +""" |
| 24 | + |
| 25 | +from math import pi |
| 26 | + |
| 27 | +import numpy as np |
| 28 | +from scipy.fft import fft, fft2, fftshift, ifft, ifft2, ifftshift |
| 29 | + |
| 30 | + |
| 31 | +def fresnel_diffract( |
| 32 | + wavefunc_0: np.ndarray, pixel_size: float, wavelength: float, prop_dist: float |
| 33 | +) -> np.ndarray: |
| 34 | + """ |
| 35 | + Fresnel Diffraction of 1D or 2D Wave Fields. |
| 36 | +
|
| 37 | + This function calculates the Fresnel diffraction of a |
| 38 | + given wave field, suitable for near-field diffraction. The |
| 39 | + wave field is assumed to be coherent and monochromatic. |
| 40 | +
|
| 41 | + Args: |
| 42 | + wavefunc0 (np.ndarray): The initial wave field at the unpropagated plane. |
| 43 | + pixel_size (float): The physical size of a pixel (or data point) at the |
| 44 | + pixel_size (float): The physical size of a pixel (or data point) at the |
| 45 | + unpropagated plane. |
| 46 | + wavelength (float): The wavelength of the wave field. |
| 47 | + prop_dist (float): The desired propagation distance. |
| 48 | +
|
| 49 | + Raises: |
| 50 | + ValueError: If the input wave field is not 1D or 2D. |
| 51 | +
|
| 52 | + Returns: |
| 53 | + np.ndarray: The wave field at the propagated plane. |
| 54 | +
|
| 55 | + Examples: |
| 56 | + >>> import numpy as np |
| 57 | + >>> res = fresnel_diffract(np.ones(64), 1, 1, 1) |
| 58 | + >>> res.shape |
| 59 | + (64,) |
| 60 | + >>> import numpy as np |
| 61 | + >>> res = fresnel_diffract(np.ones((64, 64)), 1, 1, 1) |
| 62 | + >>> res.shape |
| 63 | + (64, 64) |
| 64 | + >>> import numpy as np |
| 65 | + >>> res = fresnel_diffract(np.ones((4, 4, 4)), 1, 1, 1) |
| 66 | + Traceback (most recent call last): |
| 67 | + ... |
| 68 | + ValueError: Expected a 1D or 2D wavefield, but got (4, 4, 4) |
| 69 | +
|
| 70 | + # Test that conservation of energy is obeyed |
| 71 | + >>> import numpy as np |
| 72 | + >>> wf0 = np.ones(64) |
| 73 | + >>> wfz = fresnel_diffract(wf0, 1, 1, 1) |
| 74 | + >>> bool(np.isclose(np.sum(abs(wf0)**2), np.sum(abs(wfz)**2))) |
| 75 | + True |
| 76 | + >>> import numpy as np |
| 77 | + >>> wf0 = np.ones((64, 64)) |
| 78 | + >>> wfz = fresnel_diffract(wf0, 1, 1, 1) |
| 79 | + >>> bool(np.isclose(np.sum(abs(wf0)**2), np.sum(abs(wfz)**2))) |
| 80 | + True |
| 81 | +
|
| 82 | + # Test that propagation distance of 0 returns the contact image |
| 83 | + >>> import numpy as np |
| 84 | + >>> x = np.linspace(-32, 32, 1) |
| 85 | + >>> wf0 = np.where(abs(x)<=8, 1, 0) |
| 86 | + >>> wfz = fresnel_diffract(wf0, 1, 1, 0) |
| 87 | + >>> np.allclose(wf0, wfz) |
| 88 | + True |
| 89 | + """ |
| 90 | + |
| 91 | + if len(wavefunc_0.shape) == 1: |
| 92 | + return _fresnel_diffract_1d(wavefunc_0, pixel_size, wavelength, prop_dist) |
| 93 | + elif len(wavefunc_0.shape) == 2: |
| 94 | + return _fresnel_diffract_2d(wavefunc_0, pixel_size, wavelength, prop_dist) |
| 95 | + else: |
| 96 | + error_message = f"Expected a 1D or 2D wavefield, but got {wavefunc_0.shape}" |
| 97 | + raise ValueError(error_message) |
| 98 | + |
| 99 | + |
| 100 | +def _fresnel_diffract_2d( |
| 101 | + wavefunc_0: np.ndarray, pixel_size: float, wavelength: float, prop_dist: float |
| 102 | +) -> np.ndarray: |
| 103 | + """ |
| 104 | + Fresnel Diffraction of 2D Wave Fields. |
| 105 | + This private function is called by 'fresnel_diffract' to handle the |
| 106 | + fresnel diffraction of 2D wave fields specifically. |
| 107 | + Args: |
| 108 | + wavefunc_0 (np.ndarray): The initial 2D wave field at the unpropagated plane. |
| 109 | + pixel_size (float): The physical size of a pixel (or data point) at the |
| 110 | + unpropagated plane. |
| 111 | + wavelength (float): The wavelength of the wave field. |
| 112 | + prop_dist (float): The desired propagation distance. |
| 113 | +
|
| 114 | + Returns: |
| 115 | + np.ndarray: The 2D wave field at the propagated plane. |
| 116 | +
|
| 117 | +
|
| 118 | + Examples: |
| 119 | + >>> import numpy as np |
| 120 | + >>> res = _fresnel_diffract_2d(np.ones((64, 64)), 1, 1, 1) |
| 121 | + >>> res.shape |
| 122 | + (64, 64) |
| 123 | + >>> import numpy as np |
| 124 | + >>> wf0 = np.ones((64, 64)) |
| 125 | + >>> wfz = _fresnel_diffract_2d(wf0, 1, 1, 1) |
| 126 | + >>> bool(np.isclose(np.sum(abs(wf0)**2), np.sum(abs(wfz)**2))) |
| 127 | + True |
| 128 | +
|
| 129 | + # Test that propagation distance of 0 returns the contact image |
| 130 | + >>> import numpy as np |
| 131 | + >>> x = np.linspace(-32, 32, 1) |
| 132 | + >>> X1, X2 = np.meshgrid(x, x) |
| 133 | + >>> wf0 = np.where(abs(X1)<=8, 1, 0) * np.where(abs(X2)<=8, 1, 0) |
| 134 | + >>> wfz = _fresnel_diffract_2d(wf0, 1, 1, 0) |
| 135 | + >>> np.allclose(wf0, wfz) |
| 136 | + True |
| 137 | + """ |
| 138 | + pixel_num, _ = wavefunc_0.shape |
| 139 | + side_length = pixel_num * pixel_size |
| 140 | + |
| 141 | + # Coordinates in Fourier space are proportionate to 1 / pixel_size |
| 142 | + f_x = np.arange(-1 / (2 * pixel_size), 1 / (2 * pixel_size), 1 / side_length) |
| 143 | + |
| 144 | + f_x2d, f_y2d = np.meshgrid(f_x, f_x) |
| 145 | + |
| 146 | + # Transfer function which models diffraction |
| 147 | + transferf = np.exp(-1j * np.pi * wavelength * prop_dist * (f_x2d**2 + f_y2d**2)) |
| 148 | + transferf = fftshift(transferf) |
| 149 | + |
| 150 | + # Fourier space wave function at the unpropagated plane |
| 151 | + f_wavefunc_0 = fft2(fftshift(wavefunc_0)) |
| 152 | + # Wave function at the propagated, or 'z' plane |
| 153 | + wavefuncz = ifftshift(ifft2(transferf * f_wavefunc_0)) |
| 154 | + |
| 155 | + return wavefuncz |
| 156 | + |
| 157 | + |
| 158 | +def _fresnel_diffract_1d( |
| 159 | + wavefunc_0: np.ndarray, pixel_size: float, wavelength: float, prop_dist: float |
| 160 | +) -> np.ndarray: |
| 161 | + """ |
| 162 | + Fresnel Diffraction of 1D Wave Fields. |
| 163 | + This private function is called by 'fresnel_diffract' to handle the |
| 164 | + fresnel diffraction of 1D wave fields specifically. |
| 165 | + Args: |
| 166 | + wavefunc0 (np.ndarray): The initial 1D wave field at the unpropagated plane. |
| 167 | + pixel_size (float): The physical size of a pixel (or data point) at the |
| 168 | + unpropagated plane. |
| 169 | + wavelength (float): The wavelength of the wave field. |
| 170 | + prop_dist (float): The desired propagation distance. |
| 171 | +
|
| 172 | + Returns: |
| 173 | + np.ndarray: The 1D wave field at the propagated plane. |
| 174 | +
|
| 175 | +
|
| 176 | + Examples: |
| 177 | + >>> import numpy as np |
| 178 | + >>> res = _fresnel_diffract_1d(np.ones(64), 1, 1, 1) |
| 179 | + >>> res.shape |
| 180 | + (64,) |
| 181 | +
|
| 182 | + # Conservation of energy |
| 183 | + >>> import numpy as np |
| 184 | + >>> wf0 = np.ones(64) |
| 185 | + >>> wfz = _fresnel_diffract_1d(wf0, 1, 1, 1) |
| 186 | + >>> bool(np.isclose(np.sum(abs(wf0)**2), np.sum(abs(wfz)**2))) |
| 187 | + True |
| 188 | +
|
| 189 | + # Test that propagation distance of 0 returns the contact image |
| 190 | + >>> import numpy as np |
| 191 | + >>> x = np.linspace(-32, 32, 1) |
| 192 | + >>> wf0 = np.where(abs(x)<=8, 1, 0) |
| 193 | + >>> wfz = _fresnel_diffract_1d(wf0, 1, 1, 0) |
| 194 | + >>> np.allclose(wf0, wfz) |
| 195 | + True |
| 196 | + """ |
| 197 | + pixel_num = len(wavefunc_0) |
| 198 | + side_length = pixel_num * pixel_size |
| 199 | + fx = np.arange(-1 / (2 * pixel_size), 1 / (2 * pixel_size), 1 / side_length) |
| 200 | + transferf = np.exp(-1j * pi * wavelength * prop_dist * (fx**2)) |
| 201 | + transferf = fftshift(transferf) |
| 202 | + |
| 203 | + f_wavefunc_0 = fft(fftshift(wavefunc_0)) |
| 204 | + |
| 205 | + wavefunc_z = ifftshift(ifft(transferf * f_wavefunc_0)) |
| 206 | + |
| 207 | + return wavefunc_z |
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