Abstract

A coherence-controlled holographic microscope (CCHM) enables quantitative phase imaging with coherent as well as incoherent illumination. The low spatially coherent light induces a coherence gating effect, which makes observation of samples possible also through scattering media. The paper describes theoretically and simulates numerically imaging of a two-dimensional object through a static scattering layer by means of CCHM, with the main focus on the quantitative phase imaging quality. The authors have investigated both strongly and weakly scattering media characterized by different amounts of ballistic and diffuse light. It is demonstrated that the phase information can be revealed also for the case of the static, strongly scattering layer. The dependence of the quality of imaging process on the spatial light coherence is demonstrated. The theoretical calculations and numerical simulations are supported by experimental data gained with a model phase object, as well as living carcinoma cells treated in an optically turbid emulsion.

Highlights

  • Imaging through scattering media is an important task in biomedical as well technical research and applications

  • Digital holographic microscopy based on transmission mode has made quantitative phase imaging (QPI) of living cells and other phase objects[9,10,11,12,13] possible, and its potential and applications are further investigated

  • This paper proves the possibility of QPI of 2-D phase objects through a static phase scattering layer by means of coherence-controlled holographic microscope (CCHM)

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Summary

Introduction

Imaging through scattering media is an important task in biomedical as well technical research and applications. The imaging of an object with defined phase is numerically as well as experimentally evaluated for weak and strong diffuse layers. The quality of imaging with ballistic and diffuse light is similar in the case of strong diffusers, and mostly so noisy that the phase cannot be unwrapped. In the case of high spatial coherence and a weak diffuser, Fig. 3(d) is affected by the coherence noise, the finer details are lost, and the phase unwrapping is a more complicated task.

Quantitative Phase Imaging Through a Scattering Layer—Experiments
Without diffuser With diffuser
Experiment with Living Cells
Findings
Conclusion
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