2012
DOI: 10.1364/ol.37.002877
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Single-fiber diffuse optical time-of-flight spectroscopy

Abstract: We demonstrate interstitial diffuse optical time-of-fight spectroscopy based on a single fiber for both light delivery\ud and detection. Detector saturation due to the massive short-time reflection is avoided by ultrafast gating of a single\ud photon avalanche diode. We show that the effects of scattering and absorption are separable and that absorption\ud can be assessed independently of scattering. Measurements on calibrated liquid phantoms and subsequent Monte\ud Carlo–based evaluation illustrate that absor… Show more

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Cited by 38 publications
(36 citation statements)
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“…Thanks to this feature, a single measurement is sufficient to directly uncouple absorption from scattering contributions, thus leading -for a homogeneous medium -to the absolute quantification of both absorption and reduced scattering coefficients. Further, in the case of reflectance geometry, with light source and detection points placed on the same side of the medium at a relative distance ρ, the mean penetration depth of detected photons steadily increases upon increasing the photon arrival time [39,40], thus permitting deep tissue imaging even at null-ρ [41][42][43] with the chance to reach a record level of source-detector couples coverage to maximize the detected signal and the spatial resolution, provided that an efficient time-gating mechanism is employed to avoid the blinking burst of undesired early-arriving photons [44][45][46]. However, the main limitations of TD as compared to CW systems during the last two decades have always been high cost and complexity, thus affecting the maximum number of injection and detection channels, and wider deployment of instruments for clinical use.…”
Section: Discussionmentioning
confidence: 99%
“…Thanks to this feature, a single measurement is sufficient to directly uncouple absorption from scattering contributions, thus leading -for a homogeneous medium -to the absolute quantification of both absorption and reduced scattering coefficients. Further, in the case of reflectance geometry, with light source and detection points placed on the same side of the medium at a relative distance ρ, the mean penetration depth of detected photons steadily increases upon increasing the photon arrival time [39,40], thus permitting deep tissue imaging even at null-ρ [41][42][43] with the chance to reach a record level of source-detector couples coverage to maximize the detected signal and the spatial resolution, provided that an efficient time-gating mechanism is employed to avoid the blinking burst of undesired early-arriving photons [44][45][46]. However, the main limitations of TD as compared to CW systems during the last two decades have always been high cost and complexity, thus affecting the maximum number of injection and detection channels, and wider deployment of instruments for clinical use.…”
Section: Discussionmentioning
confidence: 99%
“…Additionally, bioresorbable fibers can be profitably coupled with fast-gated detectors [39] to reject the peak of reflected or scarcely diffused photons that can saturate the dynamic range of a "classical" (i. e. non-gated) detector, thus allowing the use of a single interstitial fiber as already demonstrated in the case of classical optical fibers [40].…”
Section: Conclusion and Future Perspectivesmentioning
confidence: 99%
“…The active area is considerably smaller (20 µm -500 µm) but it is often compensated by the other advantages especially if the sample has limited emission geometry (like in confocal microscopy [9], scanning systems [10] or fiber-based endoscopy [11]). …”
Section: Introductionmentioning
confidence: 99%