Gate-readout and a 3D rectification effect for giant responsivity enhancement of asymmetric dual-grating-gate plasmonic terahertz detectors

Author:

Satou Akira1ORCID,Negoro Takumi12,Narita Kenichi12,Hosotani Tomotaka12,Tamura Koichi12,Tang Chao13ORCID,Lin Tsung-Tse1,Retaux Paul-Etienne14,Takida Yuma5,Minamide Hiroaki5,Suemitsu Tetsuya6,Otsuji Taiichi1

Affiliation:

1. Research Institute of Electrical Communication , Tohoku University , Sendai 980-8577 , Japan

2. School of Engineering , Tohoku University , Sendai , 980-8579 , Japan

3. Frontier Research Institute for Interdisciplinary Sciences , Tohoku University , Sendai , 980-8578 , Japan

4. Department of Electrical and Computer Engineering , Ecole Nationale Supérieure de l’Electronique et de ses Applications , 95000 Cergy , France

5. RIKEN Center for Advanced Photonics , RIKEN , Sendai , Miyagi , 980-0845 , Japan

6. New Industry Creation Hatchery Center , Tohoku University , Sendai 980-8579 , Japan

Abstract

Abstract We experimentally investigated the asymmetric dual-grating-gate plasmonic terahertz (THz) detector based on an InGaAs-channel high-electron-mobility transistor (HEMT) in the gate-readout configuration. Throughout the THz pulse detection measurement on the fabricated device, we discovered a new detection mechanism called the “3D rectification effect” at the positive gate bias application, which is a cooperative effect of the plasmonic nonlinearities in the channel with the diode nonlinearity in the heterobarrier between the InGaAs channel layer and the InAlAs spacer/carrier-supply/barrier layers, resulting in a giant enhancement of the detector responsivity. We also found that an undesired long-tail waveform observed on the temporal pulse photoresponse of the device is due to trapping of carriers to the donor levels in the silicon δ-doped carrier-supply layer when they tunnel through the barrier to the gate and can be eliminated completely by introducing the so-called inverted-HEMT structure. The internal current responsivity and noise-equivalent power are estimated to be 0.49 A/W (with the equivalent voltage responsivity of 4.9 kV/W with a high output impedance of 10 kΩ) and 196 pW/√Hz at 0.8 THz. These results pave the way towards the application of the plasmonic THz detectors to beyond-5G THz wireless communication systems.

Funder

Japan Society for the Promotion of Science

National Institute of Information and Communications Technology

Publisher

Walter de Gruyter GmbH

Subject

Electrical and Electronic Engineering,Atomic and Molecular Physics, and Optics,Electronic, Optical and Magnetic Materials,Biotechnology

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