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Long-wavelength metal-semiconductor-metal photodetectors with transparent and opaque electrodes

机译:具有透明和不透明电极的长波长金属半导体 - 金属光电探测器

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In this paper, we present a comparative study of transparent and opaque electrode InAlAs/InGaAs metal-semiconductor-metal photodiodes (MSMPDs) for operation at 1.31 and 1.55 $mu@m. The transparent materials are indium-tin-oxide (ITO) and cadmium-tin-oxide (CTO) and the opaque material is Ti-Au. The rf magnetron sputtered films of ITO and CTO, deposited at a substrate temperature of 300 degrees C, exhibited as-deposited resistivities of 5.6$DOT@10$+$MIN@3$/ approximately ega$DOT@cm and 1.0$DOT@10$+$MIN@3$/ approximately ega$DOT@cm, respectively. The resistivity of the ITO and CTO films dropped to 1.1$DOT@10$+$MIN@3$/ approximately ega$DOT@cm and 5.2$DOT@10$+$MIN@4$/ approximately ega$DOT@cm, respectively, after a 4 minute 400 degree C anneal in an N$-2$/ ambient. The interdigitated ITO and CTO electrodes were made by etching in a methane:hydrogen (1 to 3) plasma. The responsivity of 1 $mu@m finger by 1 $mu@m spacing (1 by 1 $mu@m), 50 $MUL 50 $mu@m$+2$/ active area, MSMPDs was 0.40 A/W for the Ti-Au, 0.66 A/W for the CTO, and 0.69 A/W for the ITO MSMPDs. The Ti-Au, CTO and ITO MSMPDs had 3- dB cut-off frequencies of 14.0 GHz, 7.5 GHz, and 5.0 GHz, respectively, from time-domain measurements performed at 1.3 $mu@m and 11.26 GHz, 4.00 GHz, and 2.61 GHz, respectively, from frequency-domain measurements performed at 1.55 $mu@m. Discrepencies between the 3-dB cut-off frequency obtained from the time-domain and the frequency-domain measurements are attributed to the time-domain measurement system's inability to accurately resolve low frequency behavior (below 2 GHz) and space charge effects.
机译:在本文中,我们介绍了透明和不透明电极Inalas / InGaAs金属 - 半导体 - 金属光电二极管(MSMPDS)的比较研究,用于在1.31和1.55 $ MU @ M处操作。透明材料是氧化铟锡(ITO)和镉 - 氧化锡(CTO),并且不透明材料是Ti-Au。 ITO和CTO的RF磁控溅射膜,沉积在300摄氏度的底物温度下,展示了5.6 /张$ + $最小的沉积电阻@ 3 $ /约EGA $ DOT @ cm和1.0 $ DOT @ 10 $ + MIN @ 3 $ /约为ega $ dot @ cm。 ITO和CTO薄膜的电阻率降至1.1 / tem $ + $ min @ 3 $ /大约ega $ dot @ cm和5.2?10 $ + $ min @ 4 $ /大约ega $ dot @ cm,分别在4分400度C退火后,在N $ -2 $ /环境中退火。通过在甲烷中蚀刻来制备交叉的ITO和CTO电极:氢气(1至3)等离子体。 1 $ mu @ m finger 1 $ mu @ m间距的响应度(1到1 $ mu @ m),50 $ mul 50 $ mu @ m $ + 2 $ /活动区域,msmpds为0.40 A / W TI-AU,CTO 0.66 A / W,ITO MSMPDS为0.69 A / W. TI-AU,CTO和ITO MSMPDS分别具有14.0GHz,7.5 GHz和5.0GHz的3-DB截止频率,从时域测量执行,在1.3 $ MU @ M和11.26 GHz,4.00 GHz,以及2.61 GHz分别从频率域测量执行,在1.55 $ mu @ m。从时域和频域测量获得的3 dB截止频率之间的差异归因于时域测量系统无法准确地解析低频行为(低于2GHz)和空间充电效果。

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