Abstract

Confocal microscopy is an essential imaging tool for biological systems, in solid-state physics and nano-photonics. Using confocal microscopes allows performing resonant fluorescence experiments, where the emitted light has the same wavelength as the excitation laser. Theses challenging experiments are carried out under linear cross-polarization conditions, rejecting laser light from the detector. In this work we uncover the physical mechanisms that are at the origin of the yet unexplained high polarization rejection ratio which makes these measurements possible. We show in both experiment and theory that the use of a reflecting surface (i.e. the beam-splitter and mirrors) placed between the polarizer and analyzer in combination with a confocal arrangement explains the giant cross-polarization extinction ratio of 10^8 and beyond. We map the modal transformation of the polarized optical Gaussian beam. We find an intensity 'hole' in the reflected beam under cross-polarization conditions. We interpret this as a manifestation of the Imbert-Fedorov effect, which deviates the beam depending on its polarization helicity. This implies that this topological effect is amplified here from the usually observed nanometer to the micrometer scale due to our cross-polarization dark field methods. We confirm these experimental findings for a large variety of commercially available mirrors and polarization components, allowing their practical implementation in many experiments.

Highlights

  • In optical spectroscopy experiments, it is crucial to excite an emitter with a laser very close to its transition energy

  • We demonstrate that behind this general observation lies the intriguing physics of the Imbert-Fedorov effect [32,33], which deviates a reflected light beam depending on its polarization helicity

  • We have exposed a systematic experimental method based on a confocal microscopy arrangement to obtain a giant enhancement in dark-field crosspolarization extinction and by up to 3 orders of magnitude and possibly beyond

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Summary

INTRODUCTION

It is crucial to excite an emitter with a laser very close to its transition energy. Using linear crosspolarization in a confocal setup has been successfully employed as a dark-field method to carry out resonant fluorescence experiments to suppress scattered laser light, with the added benefit of high spatial resolution [17,18]. We explain the physics behind the giant enhancement of the extinction ratio by up to 7 orders of magnitude that make microscopy based on dark-field laser suppression possible. We identify two key ingredients that explain the giant amplification of the cross-polarization extinction ratio: (i) a reflecting surface (i.e., the beam splitter) placed between a polarizer and analyzer and (ii) a confocal arrangement.

CONFOCAL MICROSCOPE SETUP
CANCELLATION OF POLARIZATION LEAKAGE
MODAL TRANSFORMATION OF A REFLECTED POLARIZED GAUSSIAN BEAM
EFFECT OF CONFOCAL SPATIAL FILTERING
CONCLUSIONS
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