Abstract

Swept-laser sources offer a number of advantages for Phase-sensitive Optical Coherence Tomography (PhOCT). However, inter- and intra-sweep variability leads to calibration errors that adversely affect phase sensitivity. While there are several approaches to overcoming this problem, our preferred method is to simply calibrate every sweep of the laser. This approach offers high accuracy and phase stability at the expense of a substantial processing burden. In this approach, the Hilbert phase of the interferogram from a reference interferometer provides the instantaneous wavenumber of the laser, but is computationally expensive. Fortunately, the Hilbert transform may be approximated by a Finite Impulse-Response (FIR) filter. Here we explore the use of several FIR filter based Hilbert transforms for calibration, explicitly considering the impact of filter choice on phase sensitivity and OCT image quality. Our results indicate that the complex FIR filter approach is the most robust and accurate among those considered. It provides similar image quality and slightly better phase sensitivity than the traditional FFT-IFFT based Hilbert transform while consuming fewer resources in an FPGA implementation. We also explored utilizing the Hilbert magnitude of the reference interferogram to calculate an ideal window function for spectral amplitude calibration. The ideal window function is designed to carefully control sidelobes on the axial point spread function. We found that after a simple chromatic correction, calculating the window function using the complex FIR filter and the reference interferometer gave similar results to window functions calculated using a mirror sample and the FFT-IFFT Hilbert transform. Hence, the complex FIR filter can enable accurate and high-speed calibration of the magnitude and phase of spectral interferograms.

Highlights

  • There are a variety of extensions of Optical Coherence Tomography (OCT) that take advantage of the interferometric phase to garner additional information

  • In this article we have evaluated several Finite Impulse-Response (FIR) based methods for spectral calibration of every sweep of a swept laser in real time

  • We compared results derived from imaging a mirror with the OCT interferometer and an IFFT-FFT based Hilbert transform to those obtained from the reference interferometer and the complex FIR filter

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Summary

Introduction

There are a variety of extensions of Optical Coherence Tomography (OCT) that take advantage of the interferometric phase to garner additional information. We are interested in using a technique called Phase-sensitive Optical Coherence Tomography (PhOCT) to accomplish vibrometry with picometer sensitivities. This exquisite sensitivity is enabling 3-D vibrometry in the intact cochlea of animal models of hearing, revealing new insights into cochlea function. Swept laser sources typically have very narrow instantaneous line widths that provide long coherence length and low sensitivity rolloff as a function of depth. Likewise, they are compatible with architectures using some variant of the Mach-Zehdner interferometer and balanced detection. Swept laser sources used for OCT typically suffer sweep instabilities that lead to phase noise and reduced sensitivity

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