28.5 A 0.6V/0.9V 26.6至119.3µW ΔΣ-Based生物阻抗读出IC,信噪比101.9dB, 1/f角<0.1Hz

Tantan Zhang, Hyunwoo Son, Yuan Gao, Jingjing Lan, C. Heng
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引用次数: 4

摘要

生物阻抗(BioZ)是可穿戴医疗传感中重要的生理参数。除了固有的心脏和呼吸信息外,BioZ还可用于其他新兴应用,如无创血液状态传感[1]。传统的14-e1电极(4E)设置消除了电极组织阻抗(ETI)的影响,以牺牲用户舒适度、系统复杂性和成本为代价。另一方面,双电极(2E)设置避免了4E的不足,但只能捕获Bi0Z的相对变化,而不是其绝对值。此外,需要具有宽动态范围(DR)和高信噪比(SNR)的读出前端(RFE)来处理较小的BioZ变化(0.1 $\sim10\Omega$)和较大的基线电阻(>10k $\Omega$)。采用仪表放大器(IA)和ADC的传统RFE架构必须在分辨率、DR和噪声之间进行权衡[2,3]。虽然电流发生器(CG)中的闪烁噪声通过动态元素匹配(DEM)得到缓解[2],但参考电流(IREF)噪声问题仍未得到解决。文献[5]中提出了数字辅助基线对消和IREF相关噪声对消,有助于消除由于电流平衡仪表放大器(CBIA)信号较大而产生的IREF噪声和输入相关噪声[4]。然而,由于基线抵消产生的有限剩余电流$(I_{res})$,仍然观察到较大的噪声。
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28.5 A 0.6V/0.9V 26.6-to-119.3µW ΔΣ-Based Bio-Impedance Readout IC with 101.9dB SNR and <0.1Hz 1/f Corner
Bio-impedance (BioZ) is an important physiological parameter in wearable healthcare sensing. Besides the inherent cardiac and respiratory information, BioZ can be also used for other emerging applications such as non-invasive blood status sensing [1]. A conventiona14-e1ectrode (4E) setup eliminates the effect of electrode-tissue impedance (ETI) at the expense of user comfort, system complexity, and cost. On the other hand, a 2-electrode (2E) setup avoids short-falls of 4E but can only capture relative changes of Bi0Z instead of its absolute value. In addition, a readout front-end (RFE) with wide dynamic range (DR) and high signal-to-noise ratio (SNR) is needed to deal with small BioZ variation (0.1$\sim10\Omega$) as well as large baseline resistance (>10k$\Omega$). A conventional RFE architecture employing an instrumentation amplifier (IA) and ADC has to trade-off between resolution, DR and noise [2, 3]. Although flicker noise in the current generator (CG) is mitigated through dynamic element matching (DEM) [2], the reference current (IREF) noise issue remains unaddressed. In [5], digital-assisted baseline cancellation and IREF correlated noise cancellation are proposed, which help eliminate IREF noise and input-dependent noise [4] due to the large signal in the current-balance instrumentation amplifier (CBIA). Nevertheless, larger noise is still observed due to the finite residual current $(I_{res})$ from the baseline cancellation.
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