4.7 Article

Optimal illumination scheme for isotropic quantitative differential phase contrast microscopy

Journal

PHOTONICS RESEARCH
Volume 7, Issue 8, Pages 890-904

Publisher

OPTICAL SOC AMER
DOI: 10.1364/PRJ.7.000890

Keywords

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Categories

Funding

  1. National Natural Science Foundation of China (NSFC) [61722506, 11574152]
  2. Final Assembly 13th Five-Year Plan Advanced Research Project of China [30102070102]
  3. Equipment Advanced Research Fund of China [61404150202]
  4. National Defense Science and Technology Foundation of China [0106173]
  5. Outstanding Youth Foundation of Jiangsu Province of China [BK20170034]
  6. Key Research and Development Program of Jiangsu Province [BE2017162]
  7. 333 Engineering Research Project of Jiangsu Province [BRA2016407]
  8. Fundamental Research Funds for the Central Universities [30917011204]
  9. Open Research Fund of Jiangsu Key Laboratory of Spectral Imaging & Intelligent Sense [3091801410411]

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Differential phase contrast microscopy (DPC) provides high-resolution quantitative phase distribution of thin transparent samples under multi-axis asymmetric illuminations. Typically, illumination in DPC microscopic systems is designed with two-axis half-circle amplitude patterns, which, however, result in a non-isotropic phase contrast transfer function (PTF). Efforts have been made to achieve isotropic DPC by replacing the conventional half-circle illumination aperture with radially asymmetric patterns with three-axis illumination or gradient amplitude patterns with two-axis illumination. Nevertheless, the underlying theoretical mechanism of isotropic PTF has not been explored, and thus, the optimal illumination scheme cannot be determined. Furthermore, the frequency responses of the PTFs under these engineered illuminations have not been fully optimized, leading to suboptimal phase contrast and signal-to-noise ratio for phase reconstruction. In this paper, we provide a rigorous theoretical analysis about the necessary and sufficient conditions for DPC to achieve isotropic PTF. In addition, we derive the optimal illumination scheme to maximize the frequency response for both low and high frequencies (from 0 to 2NA(obj)) and meanwhile achieve perfectly isotropic PTF with only two-axis intensity measurements. We present the derivation, implementation, simulation, and experimental results demonstrating the superiority of our method over existing illumination schemes in both the phase reconstruction accuracy and noise-robustness. (C) 2019 Chinese Laser Press

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