基于665μW硅光电倍增管的NIRS/EEG/EIT监测基础,可穿戴功能脑成像

Jiawei Xu, M. Konijnenburg, Budi Lukita, Shuang Song, Hyunsoo Ha, Roland Van Wegberg, E. Sheikhi, M. Mazzillo, G. Fallica, W. Raedt, C. Hoof, N. V. Helleputte
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引用次数: 4

摘要

功能性脑成像被认为是了解大脑和神经系统疾病的一个强大而实用的解决方案。虽然脑电图是一种非侵入性电活动的既定方法,但电阻抗断层扫描(EIT)和近红外光谱(NIRS)可以额外测量阻抗变化和血流动力学过程。为了在没有布线开销的情况下实现可穿戴设备的长期多通道脑成像,需要低功耗本地放大器[1]来支持所有这些模式。光学血流动力学测量的主要原理是将光脉冲送入组织并测量由血液中氧含量调制的反射光(图17.8.1)。最先进的近红外集成电路通常消耗几兆瓦的功率,主要用于led满足光电二极管(pd)所需的光灵敏度。硅光电倍增管(sipv)是很有前途的替代品,因为它们在可见光和近红外范围内都具有出色的低光探测能力、响应速度和更高的探测效率[2]。因此,sipm允许更深的大脑感知深度,并有可能对具有更大光电间距的一致大脑区域进行采样。这一优势将显著减少近红外通道的数量和可穿戴近红外设备的相关功率。虽然sipm需要比pd更高的偏置电压(~ 30V),但它们可以以少几百倍的LED电流实现类似的近红外响应。这导致了低功耗近红外专用集成电路和整体节能系统。由于SiPM的输出电流大且多变,现有的光学传感ic不适合用于SiPM。基于裁剪的校准方法[3]随着时间的推移存在漂移。通过交换积分器电容进行自动调零[4][5]补偿环境光,但代价是积分器的净空。除了环境光,放大器的动态范围(DR)也受到大的近红外信号的限制,导致耗电的读出。
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A 665μW silicon photomultiplier-based NIRS/EEG/EIT monitoring asic for wearable functional brain imaging
Functional brain imaging is considered a powerful and practical solution for understanding the brain and neurological diseases. While EEG is an established method for non-invasive electrical activity, electrical-impedance tomography (EIT) and near-infrared spectroscopy (NIRS) can additionally measure impedance changes and hemodynamic processes. To facilitate long-term multi-channel brain imaging in a wearable form factor without cabling overhead, there is a need for low-power local amplifiers [1] to support all these modalities. The main principle of optical hemodynamic measurements is to send light pulses into the tissue and measure the reflected light, which is modulated by the oxygen levels in the blood (Fig. 17.8.1). State-of-the-art NIRS ICs typically consume a few mW, primarily for the LEDs to meet the required light sensitivity at the photodiodes (PDs). Silicon photomultipliers (SiPMs) are promising alternatives because they have excellent low-light detection capabilities, speed of response and higher detection efficiency in both visible and near infrared range [2]. Hence, SiPMs allow deeper brain sensing depth and the possibility to sample consistent cerebral regions with larger inter-optode distance. This benefit would significantly reduce the number of NIRS channels and the associated power for a wearable NIRS device. Although SiPMs require a higher bias voltage (∼30V) than PDs, they achieve similar NIRS responses with a few hundred times less LED current. This results in a low-power NIRS ASIC and an overall power-efficient system. Existing optical sensing ICs are not suitable for a SiPM because of its large and variable output current. Trimming-based calibration methods [3] suffer from drift over time. Auto-zeroing by swapping an integrator capacitor [4][5] compensates ambient light at the cost of the integrator's headroom. Apart from ambient light, the dynamic range (DR) of the amplifier is also limited by a large NIRS signal, leading to a power-hungry readout.
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