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. 2023 Jul 24;13(1):11982.
doi: 10.1038/s41598-023-39281-5.

Fast time-domain diffuse correlation spectroscopy with superconducting nanowire single-photon detector: system validation and in vivo results

Affiliations

Fast time-domain diffuse correlation spectroscopy with superconducting nanowire single-photon detector: system validation and in vivo results

Veronika Parfentyeva et al. Sci Rep. .

Abstract

Time-domain diffuse correlation spectroscopy (TD-DCS) has been introduced as an advancement of the "classical" continuous wave DCS (CW-DCS) allowing one to not only to measure depth-resolved blood flow index (BFI) but also to extract optical properties of the measured medium without using any additional diffuse optics technique. However, this method is a photon-starved technique, specially when considering only the late photons that are of primary interest which has limited its in vivo application. In this work, we present a TD-DCS system based on a superconducting nanowire single-photon detector (SNSPD) with a high quantum efficiency, a narrow timing response, and a negligibly low dark count noise. We compared it to the typically used single-photon avalanche diode (SPAD) detector. In addition, this system allowed us to conduct fast in vivo measurements and obtain gated pulsatile BFI on the adult human forehead.

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Conflict of interest statement

A.D.M., D.C., A.T. and A.P. are cofounders of PIONIRS s.r.l. (Italy). T.D. is an inventor on relevant patents. ICFO has equity ownership in the spin-off company HemoPhotonics S.L. (Spain), potential financial conflicts of interest and objectivity of research have been monitored by ICFO’s Knowledge & Technology Transfer Department. The other authors declare no competing interests.

Figures

Figure 1
Figure 1
Experimental system (BS, beam splitter; VA, variable attenuator; PD, photodiode; MMF, multimode fiber; SMF, single mode fiber; TCSPC, time-correlated single-photon counting), schematically divided in source, detection and data acquisition units (red, grey and green boxes respectively).
Figure 2
Figure 2
Scheme on how photon arrival times are registered, windowed with overlapping segments and then processed with calculating intensity autocorrelation function.
Figure 3
Figure 3
Intralipid phantom measurement with the SPAD detector and the SNSPD: black—results from the SPAD, blue—results from the SNSPD; (a) measured normalized IRF, (b) measured DTOF, (c) ungated auto-correlation function averaged over 30 curves, shaded region represents a standard deviation.
Figure 4
Figure 4
Gated analysis of the intralipid phantom measurements with the SNSPD. (a) IRF (gray) and DTOF (blue) of the SNSPD with gates, (b) example of one g2 curve for each gate, (c) fitted αDb averaged over 30 values with standard deviation for each gate.
Figure 5
Figure 5
(a) IRF (gray), DTOF (blue), and fitted DTOF curve (red) of Subject 4 with shaded early and late gates; (b) pulsatile rBFI of Subject 4; (c) Power spectral density estimate (PSD) calculated over 7-minute of Resting state period for all 4 subjects. Colours correspond to different gates: black—ungated case, blue—early gate, red—late gate.
Figure 6
Figure 6
(a) Example of slow (bold line) and fast (thin pulsating line) rBFI signals to VM exercise (grey region highlights the VM time period); (b) rBFI response to VM exercise averaged over 6 repetitions (2 subjects × 3 repetitions), numbers show the location of each phase.

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