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High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform

The useful imaging range in spectral domain optical coherence tomography (SD-OCT) is often limited by the depth dependent sensitivity fall-off. Processing SD-OCT data with the non-uniform fast Fourier transform (NFFT) can improve the sensitivity fall-off at maximum depth by greater than 5dB concurre...

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Detalles Bibliográficos
Autores principales: Chan, Kenny K. H., Tang, Shuo
Formato: Texto
Lenguaje:English
Publicado: Optical Society of America 2010
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3018116/
https://www.ncbi.nlm.nih.gov/pubmed/21258551
http://dx.doi.org/10.1364/BOE.1.001309
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author Chan, Kenny K. H.
Tang, Shuo
author_facet Chan, Kenny K. H.
Tang, Shuo
author_sort Chan, Kenny K. H.
collection PubMed
description The useful imaging range in spectral domain optical coherence tomography (SD-OCT) is often limited by the depth dependent sensitivity fall-off. Processing SD-OCT data with the non-uniform fast Fourier transform (NFFT) can improve the sensitivity fall-off at maximum depth by greater than 5dB concurrently with a 30 fold decrease in processing time compared to the fast Fourier transform with cubic spline interpolation method. NFFT can also improve local signal to noise ratio (SNR) and reduce image artifacts introduced in post-processing. Combined with parallel processing, NFFT is shown to have the ability to process up to 90k A-lines per second. High-speed SD-OCT imaging is demonstrated at camera-limited 100 frames per second on an ex-vivo squid eye.
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spelling pubmed-30181162011-01-21 High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform Chan, Kenny K. H. Tang, Shuo Biomed Opt Express Optical Coherence Tomography The useful imaging range in spectral domain optical coherence tomography (SD-OCT) is often limited by the depth dependent sensitivity fall-off. Processing SD-OCT data with the non-uniform fast Fourier transform (NFFT) can improve the sensitivity fall-off at maximum depth by greater than 5dB concurrently with a 30 fold decrease in processing time compared to the fast Fourier transform with cubic spline interpolation method. NFFT can also improve local signal to noise ratio (SNR) and reduce image artifacts introduced in post-processing. Combined with parallel processing, NFFT is shown to have the ability to process up to 90k A-lines per second. High-speed SD-OCT imaging is demonstrated at camera-limited 100 frames per second on an ex-vivo squid eye. Optical Society of America 2010-11-04 /pmc/articles/PMC3018116/ /pubmed/21258551 http://dx.doi.org/10.1364/BOE.1.001309 Text en ©2010 Optical Society of America http://creativecommons.org/licenses/by-nc-nd/3.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution-Noncommercial-No Derivative Works 3.0 Unported License, which permits download and redistribution, provided that the original work is properly cited. This license restricts the article from being modified or used commercially.
spellingShingle Optical Coherence Tomography
Chan, Kenny K. H.
Tang, Shuo
High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform
title High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform
title_full High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform
title_fullStr High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform
title_full_unstemmed High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform
title_short High-speed spectral domain optical coherence tomography using non-uniform fast Fourier transform
title_sort high-speed spectral domain optical coherence tomography using non-uniform fast fourier transform
topic Optical Coherence Tomography
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3018116/
https://www.ncbi.nlm.nih.gov/pubmed/21258551
http://dx.doi.org/10.1364/BOE.1.001309
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