Spectrally-sampled OCT for sensitivity improvement from limited optical power
Although high optical illumination power is favored in optical coherence tomography (OCT) for better signal-to-noise ratio, optical power is often limited by a damaged threshold for biomedical living tissues and autocorrelation signals observed in tomograms. In order to improve signal sensitivity wi...
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Published in | Optics express Vol. 16; no. 22; p. 17457 |
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Main Authors | , , , , , , , , |
Format | Journal Article |
Language | English |
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United States
27.10.2008
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Abstract | Although high optical illumination power is favored in optical coherence tomography (OCT) for better signal-to-noise ratio, optical power is often limited by a damaged threshold for biomedical living tissues and autocorrelation signals observed in tomograms. In order to improve signal sensitivity without increasing the optical illumination power, a spectrally sampled multi-wavelength light source is proposed for the OCT system. A fiber Sagnac comb filter was used to spectrally sample the output of a continuous spectral light source. Point spread function analysis shows that the spectrally sampled OCT has an almost 50% dynamic range improvement in comparison with a conventional continuous spectral light source OCT for the same average optical power of 6 mW. |
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AbstractList | Although high optical illumination power is favored in optical coherence tomography (OCT) for better signal-to-noise ratio, optical power is often limited by a damaged threshold for biomedical living tissues and autocorrelation signals observed in tomograms. In order to improve signal sensitivity without increasing the optical illumination power, a spectrally sampled multi-wavelength light source is proposed for the OCT system. A fiber Sagnac comb filter was used to spectrally sample the output of a continuous spectral light source. Point spread function analysis shows that the spectrally sampled OCT has an almost 50% dynamic range improvement in comparison with a conventional continuous spectral light source OCT for the same average optical power of 6 mW. |
Author | Eom, Tae Joong Kim, Moon Ki Jeong, Myung Yung Park, Jae-Seok Kim, Chang-Seok Lee, Jongmin Yu, Bong-Ahn Jung, Eun Joo Gee, Sangyoun |
Author_xml | – sequence: 1 givenname: Eun Joo surname: Jung fullname: Jung, Eun Joo organization: Department of Nanosystem Engineering, Pusan National University, Busan, Korea – sequence: 2 givenname: Jae-Seok surname: Park fullname: Park, Jae-Seok – sequence: 3 givenname: Myung Yung surname: Jeong fullname: Jeong, Myung Yung – sequence: 4 givenname: Chang-Seok surname: Kim fullname: Kim, Chang-Seok – sequence: 5 givenname: Tae Joong surname: Eom fullname: Eom, Tae Joong – sequence: 6 givenname: Bong-Ahn surname: Yu fullname: Yu, Bong-Ahn – sequence: 7 givenname: Sangyoun surname: Gee fullname: Gee, Sangyoun – sequence: 8 givenname: Jongmin surname: Lee fullname: Lee, Jongmin – sequence: 9 givenname: Moon Ki surname: Kim fullname: Kim, Moon Ki |
BackLink | https://www.ncbi.nlm.nih.gov/pubmed/18958028$$D View this record in MEDLINE/PubMed |
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