Abstract

.Significance: The ability of diffuse correlation spectroscopy (DCS) to measure cerebral blood flow (CBF) in humans is hindered by the low signal-to-noise ratio (SNR) of the method. This limits the high acquisition rates needed to resolve dynamic flow changes and to optimally filter out large pulsatile oscillations and prevents the use of large source-detector separations (), which are needed to achieve adequate brain sensitivity in most adult subjects.Aim: To substantially improve SNR, we have built a DCS device that operates at 1064 nm and uses superconducting nanowire single-photon detectors (SNSPD).Approach: We compared the performances of the SNSPD-DCS in humans with respect to a typical DCS system operating at 850 nm and using silicon single-photon avalanche diode detectors.Results: At a 25-mm separation, we detected times more photons and achieved an SNR gain of on the forehead of 11 subjects using the SNSPD-DCS as compared to typical DCS. At this separation, the SNSPD-DCS is able to detect a clean pulsatile flow signal at 20 Hz in all subjects. With the SNSPD-DCS, we also performed measurements at 35 mm, showing a lower scalp sensitivity of with respect to the scalp sensitivity at 25 mm for both the 850 and 1064 nm systems. Furthermore, we demonstrated blood flow responses to breath holding and hyperventilation tasks.Conclusions: While current commercial SNSPDs are expensive, bulky, and loud, they may allow for more robust measures of non-invasive cerebral perfusion in an intensive care setting.

Highlights

  • Diffuse correlation spectroscopy (DCS) is a non-invasive optical method for the measurement of blood flow (BF).[1]

  • Using a fiber Mach–Zehnder interferometer and conventional silicon single-photon avalanche photodiodes (SPAD) detectors, we have shown an increase in the signalto-noise ratio (SNR) of the autocorrelation curve by a factor of ∼2 and a reduction of 80% in the coefficient of variation of the fitted BFi at long sourcedetector separations (>30 mm).[7]

  • superconducting nanowire single-photon detectors (SNSPD)-DCS collected an order of magnitude more photons than conventional DCS and for τ 1⁄4 4 μs we achieved an SNR gain of 16 Æ 8

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Summary

Introduction

Diffuse correlation spectroscopy (DCS) is a non-invasive optical method for the measurement of blood flow (BF).[1] In DCS, the tissue is illuminated by a long coherence length near-infrared laser, and the speckle pattern formed by moving scatterers, mostly red blood cells, modulates Neurophotonics. Ozana et al.: Superconducting nanowire single-photon sensing of cerebral blood flow the detected light. To maximize the contrast of the measured speckle, single-mode fibers are used, greatly limiting potential photon throughput. Current DCS devices employing single-photon avalanche photodiodes (SPAD) detectors and laser sources at 700 to 850 nm typically operate at a source-detector (SD) separation of 25 mm and an acquisition rate of 1 Hz.[3] Larger SD separations are desirable for improving brain sensitivity and reducing scalp signal contamination, especially in the adult population. Faster acquisition rates are needed to detect fast BF dynamics and effectively remove the large pulsatile systemic component from the cerebral signals. The low signalto-noise ratio (SNR) of current devices limits the acquisition rates and prevents the use of SD separations >2.5 cm

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