Abstract

We report on a theoretical model for image formation in full-field optical coherence tomography (FFOCT). Because the spatial incoherence of the illumination acts as a virtual confocal pinhole in FFOCT, its imaging performance is equivalent to a scanning time-gated coherent confocal microscope. In agreement with optical experiments enabling a precise control of aberrations, FFOCT is shown to have nearly twice the resolution of standard imaging at moderate aberration level. Beyond a rigorous study on the sensitivity of FFOCT with respect to aberrations, this theoretical model paves the way towards an optimized design of adaptive optics and computational tools for high-resolution and deep imaging of biological tissues.

Highlights

  • Since the early nineties, optical coherence tomography (OCT) has become a widely used imaging technique in medical science especially in ophthalmology

  • full-field optical coherence tomography (FFOCT) is shown to be equivalent to a time-gated confocal microscope where the scanner acts synchronously on the sample arm and on the reference arm

  • These experimental results are interpreted by means of a simple Fourier optics model that allows to compare FFOCT with other standard reflection imaging techniques

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Summary

INTRODUCTION

Optical coherence tomography (OCT) has become a widely used imaging technique in medical science especially in ophthalmology. Structured [16] or spatially-incoherent [17] illuminations can be used to maintain the confocal gate of the original FFOCT scheme [8, 9] and filter most of multiple scattering background Whether it be recorded in the time or spectral domains, studying the impact of aberrations on the FFOCT image formation is crucial to understand how to incorporate efficient adaptive optics [18, 19] or post-processing computational tools such as interferometric synthetic aperture microscopy [14, 20,21,22] or matrix imaging methods [23, 24] in FFOCT [25]. We will conclude on how adaptive optics and matrix imaging methods can help, in the near future, on how to overcome the aforementioned issues

EXPERIMENTAL RESULTS
ANALYTICAL MODEL
SAMPLE ARM c
Incident wave-field
Reflected wave-field in the sample arm
Standard incoherent image
FFOCT image
DIFFRACTION-LIMITED RESOLUTION
ROBUSTNESS TO DEFOCUS
Defocus in a conventional microscope
Amplitude transfer function for a spatially-incoherent illumination
Point-spread function for a spatially-incoherent illumination
Point-spread function for a partially coherent illumination
Coherent object
LOW-ORDER ABERRATIONS
Odd phase pupil function
Even phase pupil function
Random phase object
General case
HIGH-ORDER ABERRATIONS
VIII. DISCUSSION
CONCLUSION
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