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High-speed spectral-domain optical coherence tomography at 1.3 µm wavelength

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Abstract

We demonstrate a high-speed spectral domain optical coherence tomography (SD-OCT) system capable of acquiring individual axial scans in 24.4 µs at a rate of 19,000 axial scans per second, using an InGaAs line scan camera and broadband light source centered at 1.31 µm. Sensitivity of >105 dB over a 2-mm depth range was obtained with a free-space axial resolution of 12–14 µm, in agreement with our signal-to-noise ratio predictions. Images of human tissue obtained in vivo with SD-OCT show similar penetration depths to those obtained with state-of-the-art time domain OCT despite the ten-fold higher image acquisition speed. These results demonstrate the potential of 1.3 µm SD-OCT for high-speed and high-sensitivity imaging in patients.

©2003 Optical Society of America

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Figures (4)

Fig. 1.
Fig. 1. Schematic of the experimental setup. PC, polarization controller; GM, galvanometer-mounted mirror; DG, diffraction grating; FL, focusing lens; LSC, InGaAs line scan camera; DAQ, data acquisition board.
Fig. 2.
Fig. 2. Typical point spread function obtained with a partial reflector with -55 dB reflectivity (curve A, black); noise floor measured with the reference light only (curve B, red); camera read out noise (curve C, green). All the curves were obtained by averaging over 500 consecutive measurements to facilitate comparison.
Fig. 3.
Fig. 3. (a) Sensitivity measured as a function of depth (circles, black dotted line); theoretical fit (curve A’, green); theoretical sensitivity for shot-noise-limited SD-OCT (curve B’, red) and TD-OCT (curve C’, blue). (b) Axial resolution measured as the FWHM
Fig. 4.
Fig. 4. (a) Image of a human finger acquired in vivo with the SD-OCT system at 38 fps (256 axial×500 transverse pixels, 2.1×5.0 mm). (b) Image of the same human finger (250 axial×500 transverse pixels, 2.5×5.0 mm) acquired at 4 fps using a state-of-the-art TD-OCT system. The scale bars represent 0.5 mm.

Equations (2)

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S [ d B ] = 10 × log ( N s 1 + N el 2 N ref + α ( f Δ ν ) N ref ) ,
R ( z ) = ( sin ζ ζ ) 2 · exp [ w 2 2 ln 2 ζ 2 ] ,
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