We present a novel technique for wide dynamic range optical investigations. It is based on a fast-gated silicon singlephoton avalanche diode (SPAD) in time-correlated single-photon counting (TCSPC) setup. The SPAD is gated-ON and OFF in 500 ps so as to detect photons only within a given time interval. This technique is particularly useful in applications where a large amount of unnecessary photons precede or follow the optical signal to be detected, such as in time-resolved near infrared (NIR) spectroscopy, optical mammography, and optical molecular imaging. In particular, in time-resolved reflectance spectroscopy, it is desirable to minimize the source-detector separation to improve system performance. This leads to the saturation of the detection electronics because of the huge amount of "early" photons back scattered by superficial layers. Our setup is able to reject these photons and detect only "late" photons from the sample, thus allowing an increase in the dynamic range and the injected power.We acquired diffusive curves of two phantomswith 95 ps time resolution and 107 dynamic range with a measurement time three orders of magnitude shorter than what is currently possible with a standard TCPSC setup.
Fast-gated single photon avalanche diode for wide dynamic range NIR spectroscopy
A Pifferi;L Spinelli;R Cubeddu
2010
Abstract
We present a novel technique for wide dynamic range optical investigations. It is based on a fast-gated silicon singlephoton avalanche diode (SPAD) in time-correlated single-photon counting (TCSPC) setup. The SPAD is gated-ON and OFF in 500 ps so as to detect photons only within a given time interval. This technique is particularly useful in applications where a large amount of unnecessary photons precede or follow the optical signal to be detected, such as in time-resolved near infrared (NIR) spectroscopy, optical mammography, and optical molecular imaging. In particular, in time-resolved reflectance spectroscopy, it is desirable to minimize the source-detector separation to improve system performance. This leads to the saturation of the detection electronics because of the huge amount of "early" photons back scattered by superficial layers. Our setup is able to reject these photons and detect only "late" photons from the sample, thus allowing an increase in the dynamic range and the injected power.We acquired diffusive curves of two phantomswith 95 ps time resolution and 107 dynamic range with a measurement time three orders of magnitude shorter than what is currently possible with a standard TCPSC setup.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.