Broadband terahertz radiation from a biased two-dimensional electron gas in an AlGaN/GaN heterostructure  

Broadband terahertz radiation from a biased two-dimensional electron gas in an AlGaN/GaN heterostructure

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作  者:郑中信 孙建东 周宇 张志鹏 秦华 

机构地区:[1]Key Laboratory of Nanodevices and Applications,Suzhou Institute of Nano-Tech and Nano-Bionics,Chinese Academy of Sciences [2]University of Chinese Academy of Sciences

出  处:《Journal of Semiconductors》2015年第10期55-59,共5页半导体学报(英文版)

基  金:Project supported by the National Basic Research Program of China(No.G2009CB929303);the National Natural Science Foundation of China(No.61271157);the China Postdoctoral Science Foundation(No.2014M551678);the Jiangsu Planned Projects for Postdoctoral Research Funds(No.1301054B)

摘  要:The broadband terahertz (THz) emission from drifting two-dimensional electron gas (2DEG) in an AI- GaN/GaN heterostructure at 6 K is reported. The devices are designed as THz plasmon emitters according to the Smith-Purcell effect and the 'shallow water' plasma instability mechanism in 2DEG. Plasmon excitation is excluded since no signature of electron-density dependent plasmon mode is observed. Instead, the observed THz emission is found to come from the heated lattice and/or the hot electrons. Simulated emission spectra of hot electrons taking into account the THz absorption in air and Fabry-Pérot interference agree well with the experiment. It is confirmed that a blackbody-like THz emission will inevitably be encountered in similar devices driven by a strong in-plane electric field. A conclusion is drawn that a more elaborate device design is required to achieve efficient plasmon excitation and THz emission.The broadband terahertz (THz) emission from drifting two-dimensional electron gas (2DEG) in an AI- GaN/GaN heterostructure at 6 K is reported. The devices are designed as THz plasmon emitters according to the Smith-Purcell effect and the 'shallow water' plasma instability mechanism in 2DEG. Plasmon excitation is excluded since no signature of electron-density dependent plasmon mode is observed. Instead, the observed THz emission is found to come from the heated lattice and/or the hot electrons. Simulated emission spectra of hot electrons taking into account the THz absorption in air and Fabry-Pérot interference agree well with the experiment. It is confirmed that a blackbody-like THz emission will inevitably be encountered in similar devices driven by a strong in-plane electric field. A conclusion is drawn that a more elaborate device design is required to achieve efficient plasmon excitation and THz emission.

关 键 词:two-dimensional electron gas hot electron blackbody radiation PLASMON Fabry-Pérot cavity 

分 类 号:O441[理学—电磁学]

 

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