基于电生物阻抗传感的贴片夹持中的生理运动补偿

Kaat Van Assche, Yao-ping Zhang, M. Ourak, Eric Verschooten, P. Joris, E. V. Poorten
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引用次数: 1

摘要

神经元的贴片夹紧是一种强大的技术,用于了解大脑的电生理信号和推进神经系统疾病的研究。在体内膜片夹紧技术中,将微移液管夹在神经元细胞体的膜上。由于神经元体积小,缺乏视觉反馈,以及由心跳和呼吸引起的生理诱导运动,因此在接近神经元方面存在挑战,因此这项技术很难且耗时。本文提出了一种基于模型的运动补偿算法,该算法完全依赖于电生物阻抗(EBI)传感。最终目标是消除膜片移液器与神经元之间的相对运动,以提高体内膜片夹紧效率。在提出的算法中,ebi移液器测量响应生理诱导的运动,用于施加移液器类似于神经元的运动。该模型基于一个假设,即生理运动可以用一个正弦模型来近似,该模型有三个参数:频率、相位和幅度。在实验装置中对所开发的补偿算法进行了评估,结果表明,对于人为施加的1 Hz, 2 Hz和3 Hz的振幅为$31\ \upmu \ mathm {m}$的运动,补偿效率为$(85.5\pm 3.6) %,(81.9\ \pm 4.0) %,(75.9\pm 1.8) %。该算法还可以根据振幅、相位和频率的变化实时调整其运动特性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Physiological Motion Compensation in Patch Clamping using Electrical Bio-impedance Sensing
Patch clamping of neurons is a powerful technique used to understand the electrophysiological signals of the brain and advance research into neurological disorders. In in vivo patch clamping, a micropipette is clamped onto the membrane of a neuronal cell body. This technique is difficult and time-consuming to perform due to the challenges in approaching neurons because of their small size, the absence of visual feedback, and physiologically induced movement caused by heartbeat and breathing. This paper presents a model-based motion compensation algorithm relying solely on electrical bio-impedance (EBI) sensing. The ultimate goal is to cancel out the relative motion between the patch-pipette and the neuron to increase in vivo patch clamping efficiency. In the proposed algorithm, EBI-pipette measurements in response to physiologically induced motions are used to impose on the pipette a motion similar to that of the neuron. The model is based on the assumption that physiological motion can be approximated by a sinusoidal model with three parameters: frequency, phase, and amplitude. The developed compensation algorithm was evaluated in an experimental setup and results yielded a compensation efficiency of $(85.5\pm 3.6)\%,(81.9\ \pm 4.0)\%,(75.9\pm 1.8)\%$ for artificially imposed motions of 1 Hz, 2 Hz and 3 Hz with an amplitude of $31\ \upmu \mathrm{m}$. The algorithm also demonstrated that it can adjust its motion characterization in real time to changes in amplitude, phase, and also frequency.
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