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基于 InAlAs/InGaAs/InAlAs 异质结构的平面蝴蝶结微波二极管中直接检测机制的竞争。

Competition between Direct Detection Mechanisms in Planar Bow-Tie Microwave Diodes on the Base of InAlAs/InGaAs/InAlAs Heterostructures.

机构信息

Center for Physical Sciences and Technology, Saulėtekio Ave. 3, LT-10257 Vilnius, Lithuania.

Vilnius Gediminas Technical University, Saulėtekio Ave. 11, LT-10223 Vilnius, Lithuania.

出版信息

Sensors (Basel). 2023 Jan 28;23(3):1441. doi: 10.3390/s23031441.

DOI:10.3390/s23031441
PMID:36772490
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9920846/
Abstract

The application of the unique properties of terahertz radiation is increasingly needed in sensors, especially in those operating at room temperature without an external bias voltage. Bow-tie microwave diodes on the base of InGaAs semiconductor structures meet these requirements. These diodes operate on the basis of free-carrier heating in microwave electric fields, which allows for the use of such sensors in millimeter- and submillimeter-wavelength ranges. However, there still exists some uncertainty concerning the origin of the voltage detected across these diodes. This work provides a more detailed analysis of the detection mechanisms in InAlAs/InGaAs selectively doped bow-tie-shaped semiconductor structures. The influence of the InAs inserts in the InGaAs layer is investigated under various illumination and temperature conditions. A study of the voltage-power characteristics, the voltage sensitivity dependence on frequency in the K range, temperature dependence of the detected voltage and its relaxation characteristics lead to the conclusion that a photo-gradient electromotive force arises in bow-tie diodes under simultaneous light illumination and microwave radiation.

摘要

太赫兹辐射的独特性质在传感器中的应用需求日益增长,特别是在那些无需外部偏置电压即可在室温下工作的传感器中。基于 InGaAs 半导体结构的蝴蝶结型微波二极管满足这些要求。这些二极管基于微波电场中的自由载流子加热工作,这使得这些传感器能够在毫米波及亚毫米波段使用。然而,对于这些二极管中检测到的电压的起源,仍然存在一些不确定性。本工作对 InAlAs/InGaAs 选择性掺杂蝴蝶结型半导体结构中的检测机制进行了更详细的分析。在不同的照明和温度条件下,研究了 InGaAs 层中的 InAs 插入物的影响。对电压-功率特性、K 波段检测电压的频率灵敏度依赖性、检测电压的温度依赖性及其弛豫特性的研究得出结论,在同时进行光照明和微波辐射的情况下,蝴蝶结二极管中会产生光梯度电动势。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/2b0973ba2877/sensors-23-01441-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/580ad97cbf4f/sensors-23-01441-g0A1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/4d718aab40ae/sensors-23-01441-g0A2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/e1fc30096e5a/sensors-23-01441-g0A3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/58ad4c94d8e0/sensors-23-01441-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/8bbce7b20e1a/sensors-23-01441-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/17485e9f4e69/sensors-23-01441-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/3eff65a55921/sensors-23-01441-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/b559131fd042/sensors-23-01441-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/ad96ddf1d02c/sensors-23-01441-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/eb8002aa57f3/sensors-23-01441-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/9d3f98473453/sensors-23-01441-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/8f4ccb75abc7/sensors-23-01441-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/c27ef5468e99/sensors-23-01441-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/2b0973ba2877/sensors-23-01441-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/580ad97cbf4f/sensors-23-01441-g0A1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/4d718aab40ae/sensors-23-01441-g0A2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/e1fc30096e5a/sensors-23-01441-g0A3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/58ad4c94d8e0/sensors-23-01441-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/8bbce7b20e1a/sensors-23-01441-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/17485e9f4e69/sensors-23-01441-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/3eff65a55921/sensors-23-01441-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/b559131fd042/sensors-23-01441-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/ad96ddf1d02c/sensors-23-01441-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/eb8002aa57f3/sensors-23-01441-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/9d3f98473453/sensors-23-01441-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/8f4ccb75abc7/sensors-23-01441-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/c27ef5468e99/sensors-23-01441-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/17c2/9920846/2b0973ba2877/sensors-23-01441-g011.jpg

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本文引用的文献

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Indirect Measurement of Electron Energy Relaxation Time at Room Temperature in Two-Dimensional Heterostructured Semiconductors.二维异质结构半导体室温下电子能量弛豫时间的间接测量
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