Presentation Information
[18p-B2-3]A fast and sensitive THz rectenna detector working with zero-bias based on the 2D Dirac-Semimetal/Insulator heterostructure
〇Chao Tang1,2, Koichi Tamura1,3, Aoi Hamada1,3, Hiroyoshi Kudo1,3, Shinnosuke Uchigasaki1,3, Yuma Takida4, Hiroaki Minamide4, Tsung-Tse Lin1,4, Akira Satou1, Taiichi Otsuji1 (1.RIEC, Tohoku Univ., 2.FRIS, Tohoku Univ., 3.School of Eng. Tohoku Univ., 4.RAP, RIKEN)
Keywords:
2D material,THz detection,rectenna
In this study, we developed a fast and sensitive terahertz (THz) detector using a Bi2Se3/h-BN heterostructure rectenna that enables detection without a cathode-anode bias. The fabrication process involved synthesizing β-Bi2Se3 via vapor-controlled liquid phase growth and h-BN via chemical vapor deposition. The Bi2Se3 flake were cleaved and transferred onto a Si/SiO2 substrate, followed by the deposition of anode electrodes and the hot transfer method to stack an h-BN flake, completing the fabrication with cathode and anode electrodes and a bow-tie antenna with metal pads. For THz detection, we employed a 0.95-THz, 500-mW-peak injection-seeded THz parametric generator (is-TPG) as the light source, with anode and cathode electrodes connected through a bias tee using a GSG RF probe. We observed a THz photovoltage peak of 20 mV at an applied electric field of 0.25 V/nm, with a 200-ps full width at half maximum (FWHM). This resulted in a responsivity of 40 mV/W under a 50-Ω load (equivalent to 400 V/W under a 50-kΩ load) and a response time of 100 ps (equivalent to 10 Gbps) at room temperature. Remarkably, we also achieved a responsivity of 20 mV/W at zero bias with the same response speed. The asymmetry in the peak photovoltage with respect to the applied bipolar electric field is attributed to the asymmetric Dirac conical dispersions of Bi2Se3, highlighting the potential for passive, high-speed THz detection using 2D semimetal devices.
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