Abstract

Optical coherence tomography (OCT) is an appealing technique for bio-imaging, medicine, and material analysis. For many applications, OCT in mid- and far-infrared (IR) leads to significantly more accurate results. Reported mid-IR OCT systems require light sources and photodetectors which operate in mid-IR range. These devices are expensive and need cryogenic cooling. Here, we report a proof-of-concept demonstration of a wavelength tunable IR OCT technique with detection of only visible range photons. Our method is based on the nonlinear interference of frequency correlated photon pairs. The nonlinear crystal, introduced in the Michelson-type interferometer, generates photon pairs with one photon in the visible and another in the IR range. The intensity of detected visible photons depends on the phase and loss of IR photons, which interact with the sample under study. This enables us to characterize sample properties and perform imaging in the IR range by detecting visible photons. The technique possesses broad wavelength tunability and yields a fair axial and lateral resolution, which can be tailored to the specific application. The work contributes to the development of versatile 3D imaging and material characterization systems working in a broad range of IR wavelengths, which do not require the use of IR-range light sources and photodetectors.

Highlights

  • Optical coherence tomography (OCT) is an appealing technique in bio-imaging [1], medicine [2] and material analysis [3]

  • A probing light beam is split into two arms by a beam splitter, and the beams are recombined after being reflected by a reference mirror and a sample

  • For many applications, including analysis of ceramics and polymers, the OCT signal is mainly hampered by the scattering

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Summary

Introduction

Optical coherence tomography (OCT) is an appealing technique in bio-imaging [1], medicine [2] and material analysis [3]. A probing light beam is split into two arms by a beam splitter, and the beams are recombined after being reflected by a reference mirror and a sample. The interference occurs, when the optical path difference between the two arms is within the coherence length lcoh of the light source. By translating the reference mirror, the reflectivity and scattering of a sample are measured at different depths. For many applications, including analysis of ceramics and polymers, the OCT signal is mainly hampered by the scattering. In this case, OCT measurements in mid- and far- IR lead to significantly more accurate results [4]

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