Ge1-ySny photoconductor structures at 1.55 μm: From advanced materials to prototype devices

被引:38
作者
Roucka, R. [1 ]
Xie, J. [1 ]
Kouvetakis, J. [1 ]
Mathews, J. [2 ]
D'Costa, V. [2 ]
Menendez, J. [2 ]
Tolle, J. [3 ]
Yu, S. -Q. [4 ,5 ]
机构
[1] Arizona State Univ, Dept Chem & Biochem, Tempe, AZ 85287 USA
[2] Arizona State Univ, Dept Phys, Tempe, AZ 85287 USA
[3] Silicon Photon Grp Inc, Gilbert, AZ 85233 USA
[4] Arizona State Univ, Ctr Nanophoton, Tempe, AZ 85287 USA
[5] Arizona State Univ, Dept Elect Engn, Tempe, AZ 85287 USA
来源
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B | 2008年 / 26卷 / 06期
基金
美国国家科学基金会;
关键词
carrier density; CMOS integrated circuits; electron mobility; germanium compounds; infrared detectors; metallisation; photoconducting devices; photodetectors; photolithography;
D O I
10.1116/1.3021024
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Prototype detector structures were fabricated on Si substrates using Ge(1-y)Sn(y) as active material for the first time. This alloy system covers the entire near-IR telecommunication spectrum and grows at a low temperature of 350 degrees C, compatible with complementary metal-oxide-semiconductor (CMOS) Si technology. Processing protocols were developed for photolithography-based patterning and subsequent etching, CMOS compatible metallization, and for the formation of low-resistivity Ohmic contacts. A first generation of devices based on as-grown Ge(1-y)Sn(y) layers was followed by a second generation incorporating ex situ rapid thermal annealing for defect reduction, as well as additional growth and processing improvements, leading to enhanced mobilities and simultaneous reduction in intrinsic carrier concentrations. While both device generations show a significant photoconductive response at 1.55 mu m, the thicker second-generation samples yield improved performance due to better confinement of deleterious defects near the interface, which increases the optically active fraction of the film.
引用
收藏
页码:1952 / 1959
页数:8
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