Abstract

A reflection phase microscope (RPM) can be equipped with the capability of depth selection by employing a gating mechanism. However, it is difficult to achieve an axial resolution close to the diffraction limit in real implementation. Here, we systematically investigated the uneven interference contrast produced by pupil transmittance of the objective lens and found that it was the main cause of the practical limit that prevents the axial resolution from reaching its diffraction limit. Then we modulated the power of illumination light to obtain a uniform interference contrast over the entire pupil. Consequently, we could achieve an axial resolution fairly close to the diffraction limit set by the experimental conditions.

Highlights

  • A reflection phase microscope (RPM) can be equipped with the capability of depth selection by employing a gating mechanism

  • The RPMs including the successive accumulation of interferograms (SAI), which rely on the spatial coherence, have demonstrated good imaging performances and shown an axial resolution near the one expected by theory, but it has been very difficult to reach the limit, for high numerical aperture (NA) imaging, in real implementations

  • We investigated the pupil transmittance of the objective lens and found that it reduced at high NA region

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Summary

Introduction

A reflection phase microscope (RPM) can be equipped with the capability of depth selection by employing a gating mechanism. This is the origin of the depth selectivity produced by the SAI process and its ability to reject the out-of-focus information, i.e., the axial resolution of the system, thoroughly depends on the uniformity of the interference contrast over all the spatial frequency components. For the case of arbitrary pathlength difference z amplitudes of the sample and the reference beam, between the two respectively, kz is arms, where ES0 and ER0 the z-component of the are constant input wavevector k , kxR is the wavevector caused by the off-axis configuration along the x-axis, and φu(k) is the angle-dependent phase mismatch between the two waves.

Results
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