正照射延伸波长In0.8Ga0.2As红外焦平面探测器 |
| |
引用本文: | 邓洪海,杨波,邵海宝,王志亮,黄静,李雪,龚海梅.正照射延伸波长In0.8Ga0.2As红外焦平面探测器[J].红外与激光工程,2018,47(5):504004-0504004(5). |
| |
作者姓名: | 邓洪海 杨波 邵海宝 王志亮 黄静 李雪 龚海梅 |
| |
作者单位: | 1.南通大学 电子信息学院,江苏 南通 226019; |
| |
基金项目: | 国家自然科学基金(61505090);南通市科技项目(GY12015010,GY12016024);江苏省六大人才项目(2016-XCL-052,2013-XCL-013);南通智能信息技术联合研究中心开放课题基金(KFKT2016A05);江苏省高校自然科学基金(15KJB150023);江苏省高等学校自然科学研究重大项目(17KJA470007) |
| |
摘 要: | 为了研究延伸波长In0.8Ga0.2As PIN短波红外探测器的温度响应光电特性,采用闭管扩散的平面型器件工艺,在金属有机化学气相外延(MOCVD)外延生长的NIN型InAs0.6P0.4/In0.8Ga0.2As/InAs0.6P0.4 buf./InP材料上制备了正照射延伸波长2561线列InGaAs红外焦平面探测器,研究了探测器在不同温度下的I-V特性、光谱响应特性和探测率。结果表明,随着温度的降低,在小偏压下,器件的正向暗电流由产生复合电流为主逐渐变为以扩散电流为主。在260~300 K温度范围内,反向电流主要由扩散电流和产生复合电流组成,当温度低于180 K时,器件的反向电流主要为隧穿电流。室温下器件响应截止波长和峰值波长分别为2.57 m和2.09 m,峰值探测率为7.25108 cmHz1/2/W,峰值响应率为0.95 A/W,量子效率为56.9%。焦平面的峰值探测率在153 K达到峰值,约为1.111011 cmHz1/2/W,响应非均匀性为5.28%。
|
关 键 词: | 延伸波长 InGaAs 红外焦平面 变温 |
收稿时间: | 2017-12-13 |
Extended-wavelength In0.8Ga0.2As IRFPA detector arrays for front-illumination |
| |
Affiliation: | 1.School of Electronics and Information,Nantong University,Nantong 226019,China;2.Key Laboratory of Infrared Imaging Materials and Detectors,Shanghai Institute of Technical Physics,Chinese Academy of Sciences,Shanghai 200083,China |
| |
Abstract: | In order to study the temperature-dependent photoelectric characteristics of the extended wavelength In0.8Ga0.2As PIN infrared detectors, based on planer process with sealed-ampoule diffusion method, front-illuminated 2561 linear planar InGaAs detector arrays were fabricated on NIN-InAs0.6P0.4/In0.8Ga0.2As/InAs0.6P0.4 buf./InP materials by metal organic chemical vapor deposition (MOCVD). And the I-V characteristics, spectral response and detectivity of the detector at different temperatures were analyzed. The results indicate that the forward dark current is dominated by the generation-recombination current and gradually becomes the diffusion current with temperature dropping. Diffusion current and generation-recombination current were the main resource of reverse current of the detector between 260 K and 300 K. The tunneling current predominated at temperature below 180 K. The cutoff wavelength and peak wavelength were 2.57 m and 2.09 m at room temperature. The peak detectivity, peak responsivity and quantum efficiency was 7.25108 cmHz1/2/W, 0.95 A/W and 56.9% respectively. Furthermore, the average peak detectivity of the detector arrays reached a peak value of 1.111011 cmHz1/2/W and the response nonuniformity was about 5.28% at 153 K. |
| |
Keywords: | |
|
| 点击此处可从《红外与激光工程》浏览原始摘要信息 |
|
点击此处可从《红外与激光工程》下载全文 |
|