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用于视网膜假体的光电二极管电路。

Photodiode circuits for retinal prostheses.

出版信息

IEEE Trans Biomed Circuits Syst. 2011 Oct;5(5):468-80. doi: 10.1109/TBCAS.2011.2144980.

DOI:10.1109/TBCAS.2011.2144980
PMID:23852178
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7453407/
Abstract

Photodiode circuits show promise for the development of high-resolution retinal prostheses. While several of these systems have been constructed and some even implanted in humans, existing descriptions of the complex optoelectronic interaction between light, photodiode, and the electrode/electrolyte load are limited. This study examines this interaction in depth with theoretical calculations and experimental measurements. Actively biased photoconductive and passive photovoltaic circuits are investigated, with the photovoltaic circuits consisting of one or more diodes connected in series, and the photoconductive circuits consisting of a single diode in series with a pulsed bias voltage. Circuit behavior and charge injection levels were markedly different for platinum and sputtered iridium-oxide film (SIROF) electrodes. Photovoltaic circuits were able to deliver 0.038 mC/cm(2) (0.75 nC/phase) per photodiode with 50- μm platinum electrodes, and 0.54-mC/cm(2) (11 nC/phase) per photodiode with 50-μ m SIROF electrodes driven with 0.5-ms pulses of light at 25 Hz. The same pulses applied to photoconductive circuits with the same electrodes were able to deliver charge injections as high as 0.38 and 7.6 mC/cm(2) (7.5 and 150 nC/phase), respectively. We demonstrate photovoltaic stimulation of rabbit retina in-vitro, with 0.5-ms pulses of 905-nm light using peak irradiance of 1 mW/mm(2). Based on the experimental data, we derive electrochemical and optical safety limits for pixel density and charge injection in various circuits. While photoconductive circuits offer smaller pixels, photovoltaic systems do not require an external bias voltage. Both classes of circuits show promise for the development of high-resolution optoelectronic retinal prostheses.

摘要

光电二极管电路在高分辨率视网膜假体的开发中显示出巨大的潜力。虽然已经构建了其中的几个系统,甚至将一些系统植入了人体,但目前对于光、光电二极管和电极/电解质负载之间复杂的光电相互作用的描述还很有限。本研究通过理论计算和实验测量深入研究了这种相互作用。本文研究了两种电路:主动偏置光电导电路和被动光伏电路,光伏电路由一个或多个串联二极管组成,光电导电路由一个串联的二极管和一个脉冲偏置电压组成。铂电极和溅射氧化铱膜(SIROF)电极的光电导电路和光伏电路的行为和注入电荷量明显不同。对于 50-μm 厚的铂电极,光伏电路每一个光电二极管可提供 0.038 mC/cm(2)(0.75 nC/相)的电荷量,对于 50-μm 厚的 SIROF 电极,每一个光电二极管可提供 0.54-mC/cm(2)(11 nC/相)的电荷量,施加在光电二极管上的光脉冲为 50-μs,频率为 25 Hz。对于相同的电极,相同的光脉冲施加在光电导电路上,可提供高达 0.38 和 0.76 mC/cm(2)(7.5 和 150 nC/相)的电荷量。我们在体外兔视网膜中演示了光伏刺激,使用峰值辐照度为 1 mW/mm(2)的 905-nm 光,光脉冲宽度为 0.5ms。根据实验数据,我们得出了各种电路的像素密度和注入电荷量的电化学和光学安全限制。虽然光电导电路提供了更小的像素,但光伏系统不需要外部偏置电压。这两种电路都为高分辨率光电视网膜假体的开发提供了前景。

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