Deep ultraviolet enhanced silicon carbide avalanche photodiodes

A. Sampath, Y. Chen, J. Smith, S. Kelley, J. Schuster, G. Garret, H. Shen, J. Campbell, M. Wraback, M. Reed
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Abstract

High sensitivity deep ultraviolet (DUV) photodetectors operating at wavelengths shorter than 280 nm are useful for various applications, including chemical and biological identification, optical wireless communications, and UV sensing systems (1). While semiconductor avalanche photodiodes (APDs) can be more compact, lower cost and more rugged than the commonly used photomultiplier tubes (PMTs), commercially available devices such as silicon (Si) single photon counting APDs have poor DUV single photon detection efficiency. In contrast, silicon carbide (SiC) APDs are ideal for high-sensitivity detection applications, as they can possess very low dark currents, small k factor, and high gain (2). However, the responsivity of these devices diminishes at wavelengths shorter than 260 nm due to increasing absorption and carrier generation in the top doped layer of this device, the short diffusion length of minority carriers in this region, and the presence of a high density of surface states.
深紫外增强碳化硅雪崩光电二极管
工作波长短于280 nm的高灵敏度深紫外(DUV)光电探测器可用于各种应用,包括化学和生物识别,光学无线通信和紫外传感系统(1)。虽然半导体雪崩光电二极管(apd)可以比常用的光电倍管(pmt)更紧凑,成本更低,更坚固,商用器件如硅(Si)单光子计数apd的DUV单光子探测效率较差。相比之下,碳化硅(SiC) apd是高灵敏度检测应用的理想选择,因为它们可以具有非常低的暗电流,小k因子和高增益(2)。然而,由于该器件的顶部掺杂层的吸收和载流子生成增加,该区域少数载流子的扩散长度短,以及表面态密度高,这些器件的响应度在短于260 nm的波长处降低。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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