@inproceedings{fd12af672aad4d22bb521ee86011ef55,
title = "A 32-channel frequency-domain fNIRS system based on silicon photomultiplier receivers",
abstract = "Frequency-domain (FD) fNIRS is attractive for non-invasive brain imaging because phase-sensitive detection leads to increased resolution and may exhibit improved robustness to motion artifacts. We present an FD-fNIRS system with silicon photomultiplier (SiPM) receivers, where the sensitivity and dynamic range approach those of a first-class continuous-wave (CW-) fNIRS system. This represents a significant step toward fully exploiting the phase degree of freedom provided by FD-fNIRS. The transmitter subsystem includes 32 channels and each supplies 12.5 mW of coherent light at both 690 and 852 nm. A dedicated radio circuit intensity-modulates each laser, and they are independently configured to operate at frequencies up to 400 MHz. The transmitters are on-off-keyed according to a user-specified pattern to mitigate shot noise and maximize dynamic range. The receiver subsystem also includes 32 channels. Each consists of a large-area (2.16-mm diameter), high-NA (0.66) fiber bundle, which carries light to a custom photo-receiver. A three-lens assembly enhances coupling between the fiber-bundle and the SiPM, and the SiPM (ON Semiconductor MICRORB-10020) converts the signal to the electrical domain. The electrical signal is amplified and down-converted to the audio spectrum, and a transformer balances the signal and provides galvanic isolation. Each of the 32 audio waveforms is digitized at 192 kS/s in a bank of commercial audio digitizers. Using a modulation frequency of 211 MHz, swept-power measurements demonstrate that the average noise-equivalent power of the SiPM photo-receivers is 20.5 fW per square root Hz, with about 6 decades of optical dynamic range. This work was funded by a research contract under Facebook{\textquoteright}s Sponsored Academic Research Agreement.",
keywords = "Diffuse optical tomography, Frequency domain, Functional imaging, Functional near-infrared imaging, Functional neuroimaging, Near infrared spectroscopy",
author = "Wathen, \{Jeremiah J.\} and Fitch, \{Michael J.\} and Pag{\'a}n, \{Vincent R.\} and Milsap, \{Griffin W.\} and McDowell, \{Emil G.\} and Lafe Spietz and Markow, \{Zachary E.\} and Trobaugh, \{Jason W.\} and Richter, \{Edward J.\} and Adam Eggebrecht and Culver, \{Joseph P.\} and Blodgett, \{David W.\} and Hendrickson, \{Scott M.\}",
note = "Funding Information: Frequency-domain (FD) fNIRS is attractive for non-invasive brain imaging because phase-sensitive detection leads to increased resolution and may exhibit improved robustness to motion artifacts. We present an FD-fNIRS system with silicon photomultiplier (SiPM) receivers, where the sensitivity and dynamic range approach those of a first-class continuous-wave (CW-) fNIRS system. This represents a significant step toward fully exploiting the phase degree of freedom provided by FD-fNIRS. The transmitter subsystem includes 32 channels and each supplies 12.5 mW of coherent light at both 690 and 852 nm. A dedicated radio circuit intensity-modulates each laser, and they are independently configured to operate at frequencies up to 400 MHz. The transmitters are on-off-keyed according to a user-specified pattern to mitigate shot noise and maximize dynamic range. The receiver subsystem also includes 32 channels. Each consists of a large-area (2.16-mm diameter), high-NA (0.66) fiber bundle, which carries light to a custom photo-receiver. A three-lens assembly enhances coupling between the fiber-bundle and the SiPM, and the SiPM (ON Semiconductor MICRORB-10020) converts the signal to the electrical domain. The electrical signal is amplified and down-converted to the audio spectrum, and a transformer balances the signal and provides galvanic isolation. Each of the 32 audio waveforms is digitized at 192 kS/s in a bank of commercial audio digitizers. Using a modulation frequency of 211 MHz, swept-power measurements demonstrate that the average noise-equivalent power of the SiPM photo-receivers is 20.5 fW per square root Hz, with about 6 decades of optical dynamic range. This work was funded by a research contract under Facebook{\textquoteright}s Sponsored Academic Research Agreement. Publisher Copyright: {\textcopyright} 2021 SPIE.; Optical Techniques in Neurosurgery, Neurophotonics, and Optogenetics 2021 ; Conference date: 06-03-2021 Through 11-03-2021",
year = "2021",
doi = "10.1117/12.2581482",
language = "English",
series = "Progress in Biomedical Optics and Imaging - Proceedings of SPIE",
publisher = "SPIE",
editor = "Yang, \{V. X. D.\} and Luo, \{Q. M.\} and Mohanty, \{S. K.\} and J. Ding and Roe, \{A. W.\} and Kainerstorfer, \{J. M.\} and L. Fu and S. Shoham",
booktitle = "Optical Techniques in Neurosurgery, Neurophotonics, and Optogenetics",
}