tb_angular_spectrum_propagate — 2D typed op

数据种类:cimagecimage

调用:fullseye.apply(img, "tb_angular_spectrum_propagate", a=0.5, b=0.5)(2-D 的模型是一张图 + 两个标量旋钮 a,b∈[0,1])

用法

复数场的精确标量自由空间传播(角谱法)。

> 以下的详细说明为原文 —— 摘要与标题已翻译。

`U(z) = IFFT{ FFT{U(0)} * exp(i*2*pi*z*sqrt(1/lambda^2 - fx^2 - fy^2)) }`

in the `exp(-i*omega*t)` convention, so a positive *distance_um*

propagates forward. Components beyond the propagating cone

(`fx^2 + fy^2 > 1/lambda^2`) are attenuated by

`exp(-2*pi*|z|*sqrt(fx^2 + fy^2 - 1/lambda^2))`, which is the physical

evanescent decay — not zeroed, so `distance_um = 0` is an *exact*

identity and the transfer function is continuous through it.

Unlike Fresnel propagation this makes no paraxial approximation: it is the

exact solution of the Helmholtz equation for a band-limited field, valid

from a fraction of a wavelength outward.

Returns a complex128 array with the same shape as *field*.

Ground truth it reproduces (measured): `distance_um = 0` returns the field

bit-identically (it short-circuits the transform pair); propagating `+z`

then `-z` returns the original to a relative L2 error of 4.3e-16 to

5.3e-16 for a band-limited field (measured on three: 64x64 random at

+/-50 um, a 64x64 Gaussian at +/-250 um, a 128x128 random at +/-500 um);

total power is conserved to between 0 and 3.5e-16 relative on the same

three. A field *with*

evanescent content does not round-trip — those components are gone by

construction, in both directions, because that is what physically happens.

*field* is a field in the space domain, not a spectrum: do not hand it

the fftshifted output of :func:complexops.cx_fft. Real input is promoted

to complex, which loses nothing.

Aliasing: the discrete transfer function is periodic, so a field that

diffracts past the array edge wraps around. The practical guard is the

usual one — pad the field so the propagated support stays inside, and keep

`pixel_pitch_um below lambda/(2*NA)`. No warning can detect this

reliably from the array alone, so none is invented.

Raises `ValueError`: *field* is not 2-D, smaller than 2x2, larger than

:data:MAX_FIELD_ELEMENTS, masked, or non-finite; non-positive or

non-finite *wavelength_um* / *pixel_pitch_um*; non-finite *distance_um*.

Typed bridge of the optics op `angular_spectrum_propagate into the 2-D evolution registry: the same implementation, called under the op(v, a, b) convention. a drives wavelength_um (default 0.55) and b drives distance_um` (default 100).

参考(示例数据・文献)

• 示例数据目录(下载 URL / 许可证) —— 2-D 用 skimage.data(BSD/公有领域)加合成图,3-D 给出真实数据源(Stanford/PDS 等)的下载 URL。

• 算子来历与参考文献 —— 该算子族所依据的研究/方法出处。

可运行的示例(实际调用该算子并已验证的样例)

• (暂无)

类型可衔接的下一个算子(可接受 cimage 作为输入)

identity · tb_cx_ifft · tb_cx_magnitude · tb_cx_phase · tb_cx_real · tb_cx_imag · tb_cx_log_magnitude · tb_cx_apply_transfer_function

同类别(typed)

tb_points_to_voxel · tb_estimate_point_normals · tb_iss_keypoints · tb_angle_3points · tb_project_points · tb_render_point_depth · tb_statistical_outlier_removal · tb_radius_outlier_removal


*Provenance: ops.py — 2D 算子登记表。本条目由 tools/opdocs.py md 自动生成(请勿手工编辑)。*

© 2026 Kazufumi Furuse — Fullseye operator documentation. Licensed under Apache-2.0.