An Approach to Direct 3D Imaging with Coherent Light

Pub Date : 2024-08-10 DOI:10.1007/s10946-024-10212-7
I. A. Artyukov, A. S. Busarov, N. L. Popov, A. V. Vinogradov
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引用次数: 0

Abstract

We consider the 3D coefficient inverse problem for parabolic wave equation. It involves determining the spatial distribution of refractive and absorption indices by processing phase diffraction patterns obtained by irradiating an object with a set of Gaussian beams. Unlike tomography and ptychography, rotation or scanning of the sample is not required. The problem is solved by expanding the wave field and the complex dielectric constant \(\varepsilon \left(\overrightarrow{r}\right)\) over the full set of Gaussian beam functions. To determine \(\varepsilon \left(\overrightarrow{r}\right),\) we obtain a nonlinear matrix equation. The condition of its solvability allows the selection of sampling frequencies by coordinates in accordance with the practical task.

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利用相干光直接进行 3D 成像的方法
我们考虑抛物面波方程的三维系数反问题。它涉及通过处理用一组高斯光束照射物体所获得的相位衍射图样来确定折射率和吸收率的空间分布。与层析成像和层析成像不同,它不需要旋转或扫描样品。解决这个问题的方法是将波场和复介电常数(\varepsilon \left(\overrightarrow{r}\right)\)扩展到全套高斯光束函数上。为了确定 (\varepsilon \left(\overrightarrow{r}\right),\),我们得到了一个非线性矩阵方程。其可解性条件允许根据实际任务按坐标选择采样频率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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