突然 MBE 生长的 HgCdTe 异质结构中的少数载流子行为

R. Sewell, J. Dell, C. Musca, L. Faraone, K. Prince
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摘要

在分子束外延 (MBE) 生长材料上制造的异质结构 HgCdTe 器件中,研究了光生少数载流子的稳态寿命。在不间断的分子束外延生长过程中,在较窄带隙吸收层(Hg/sub 1-x/Cd/sub (x)/Te, x = 0.32, /spl lambda//sub ca,80 K/ = 4.6 /spl mu/m)材料上生长了较宽带隙封顶层(Hg/sub 1-x/Cd/sub (x)/Te, x = 0.44),从而形成了一个突兀的异质界面。在 80 K 至 300 K 范围内,稳态寿命与温度的函数关系是从光电导响应率中提取的,光波长与该温度下的峰值响应率相对应。在 80 K 时,光电导体的特定检测率为 4.5 /spl times/ 10/sup 11/ cmHz/sup-1/W/sup-1/(斩波频率为 1 kHz)。在每个测量温度下,将实验测定的稳态过剩载流子寿命与 x = 0.32 且有效 n 型掺杂密度为 3.7/spl times/ 10/sup 14/ cm/sup -3/ 的材料的理论总体寿命进行比较。在低于 180 K 的温度下,测量的寿命与计算的吸收层总体寿命 /spl sim/12 /spl mu/s 一致;但在较高温度下,有证据表明存在额外的重组机制,从而降低了材料的有效寿命。结论是,当温度高于 180 K 时,窄带隙吸收层的光生载流子会在热诱导下大量进入宽带隙封顶层,从而导致探测器的响应率降低,原因是宽带隙层的过剩载流子寿命较短,掺杂程度相对较高。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Minority carrier behaviour in abrupt MBE grown HgCdTe heterostructures
Steady-state lifetime of photogenerated minority carriers has been investigated in heterostructure HgCdTe devices fabricated on molecular beam epitaxy (MBE) grown material. A wider bandgap capping layer (Hg/sub 1-x/Cd/sub (x)/Te, x = 0.44) was grown on a narrower bandgap absorbing layer (Hg/sub 1-x/Cd/sub (x)/Te, x = 0.32, /spl lambda//sub ca,80 K/ = 4.6 /spl mu/m) material in an uninterrupted MBE growth to create an abrupt heterointerface. Steady-state lifetime as a function of temperature over the range 80 K to 300 K was extracted from photoconductive responsivity at an optical wavelength corresponding to the peak responsivity at that temperature. At 80 K, the photoconductors exhibit a specific detectivity of 4.5 /spl times/ 10/sup 11/ cmHz/sup -1/W/sup -1/ (chopping frequency of 1 kHz). For each measurement temperature, the steady-state excess carrier lifetime determined experimentally was compared to the theoretical bulk lifetime for material with x = 0.32 and effective n-type doping density of 3.7/spl times/ 10/sup 14/ cm/sup -3/. For temperatures below 180 K, the measured lifetime is in agreement with the calculated bulk lifetime for the absorbing layer of /spl sim/12 /spl mu/s; however, for higher temperatures there is evidence of an additional recombination mechanism which reduces the effective lifetime in the material. It is concluded that for temperatures above 180 K. there is significant thermally induced promotion of photogenerated carriers from the narrow bandgap absorbing layer into the wide bandgap capping layer, leading to a reduction in the responsivity of the detector due Io the lower excess carrier lifetime and relatively high doping of the wide bandgap layer.
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