Terahertz light-emitting graphene-channel transistor toward single-mode lasing

A distributed feedback dual-gate graphene-channel field-effect transistor (DFB-DG-GFET) was fabricated as a current-injection terahertz (THz) light-emitting laser transistor. We observed a broadband emission in a 1–7.6-THz range with a maximum radiation power of ~10 μW as well as a single-mode emiss...

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Main Authors: Yadav Deepika, Tamamushi Gen, Watanabe Takayuki, Mitsushio Junki, Tobah Youssef, Sugawara Kenta, Dubinov Alexander A., Satou Akira, Ryzhii Maxim, Ryzhii Victor, Otsuji Taiichi
Format: Article
Language:English
Published: De Gruyter 2018-03-01
Series:Nanophotonics
Subjects:
Online Access:https://doi.org/10.1515/nanoph-2017-0106
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author Yadav Deepika
Tamamushi Gen
Watanabe Takayuki
Mitsushio Junki
Tobah Youssef
Sugawara Kenta
Dubinov Alexander A.
Satou Akira
Ryzhii Maxim
Ryzhii Victor
Otsuji Taiichi
author_facet Yadav Deepika
Tamamushi Gen
Watanabe Takayuki
Mitsushio Junki
Tobah Youssef
Sugawara Kenta
Dubinov Alexander A.
Satou Akira
Ryzhii Maxim
Ryzhii Victor
Otsuji Taiichi
author_sort Yadav Deepika
collection DOAJ
description A distributed feedback dual-gate graphene-channel field-effect transistor (DFB-DG-GFET) was fabricated as a current-injection terahertz (THz) light-emitting laser transistor. We observed a broadband emission in a 1–7.6-THz range with a maximum radiation power of ~10 μW as well as a single-mode emission at 5.2 THz with a radiation power of ~0.1 μW both at 100 K when the carrier injection stays between the lower cutoff and upper cutoff threshold levels. The device also exhibited peculiar nonlinear threshold-like behavior with respect to the current-injection level. The LED-like broadband emission is interpreted as an amplified spontaneous THz emission being transcended to a single-mode lasing. Design constraints on waveguide structures for better THz photon field confinement with higher gain overlapping as well as DFB cavity structures with higher Q factors are also addressed towards intense, single-mode continuous wave THz lasing at room temperature.
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spelling doaj.art-1fac7edf5d4744de85b9e82f4db1b8ba2022-12-21T18:35:22ZengDe GruyterNanophotonics2192-86062192-86142018-03-017474175210.1515/nanoph-2017-0106nanoph-2017-0106Terahertz light-emitting graphene-channel transistor toward single-mode lasingYadav Deepika0Tamamushi Gen1Watanabe Takayuki2Mitsushio Junki3Tobah Youssef4Sugawara Kenta5Dubinov Alexander A.6Satou Akira7Ryzhii Maxim8Ryzhii Victor9Otsuji Taiichi10Research Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanResearch Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanResearch Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanResearch Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanDepartment of Electrical and Computer Engineering, University of Texas at Austin, Austin 78712, TX, USAResearch Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanInstitute for Physics of Microstructures, Russian Academy of Sciences, Lobachevsky State University of Nizhny Novgorod, Nizhny Novgorod 603950, RussiaResearch Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanDepartment of Computer Science and Engineering, University of Aizu, Aizu-Wakamatsu 965-8580, JapanResearch Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanResearch Institute of Electrical Communication, Tohoku University, Sendai 9808577, JapanA distributed feedback dual-gate graphene-channel field-effect transistor (DFB-DG-GFET) was fabricated as a current-injection terahertz (THz) light-emitting laser transistor. We observed a broadband emission in a 1–7.6-THz range with a maximum radiation power of ~10 μW as well as a single-mode emission at 5.2 THz with a radiation power of ~0.1 μW both at 100 K when the carrier injection stays between the lower cutoff and upper cutoff threshold levels. The device also exhibited peculiar nonlinear threshold-like behavior with respect to the current-injection level. The LED-like broadband emission is interpreted as an amplified spontaneous THz emission being transcended to a single-mode lasing. Design constraints on waveguide structures for better THz photon field confinement with higher gain overlapping as well as DFB cavity structures with higher Q factors are also addressed towards intense, single-mode continuous wave THz lasing at room temperature.https://doi.org/10.1515/nanoph-2017-0106graphenelasersfar infrared or terahertzpumpingcurrent injectiondistributed-feedbackoptoelectronics
spellingShingle Yadav Deepika
Tamamushi Gen
Watanabe Takayuki
Mitsushio Junki
Tobah Youssef
Sugawara Kenta
Dubinov Alexander A.
Satou Akira
Ryzhii Maxim
Ryzhii Victor
Otsuji Taiichi
Terahertz light-emitting graphene-channel transistor toward single-mode lasing
Nanophotonics
graphene
lasers
far infrared or terahertz
pumping
current injection
distributed-feedback
optoelectronics
title Terahertz light-emitting graphene-channel transistor toward single-mode lasing
title_full Terahertz light-emitting graphene-channel transistor toward single-mode lasing
title_fullStr Terahertz light-emitting graphene-channel transistor toward single-mode lasing
title_full_unstemmed Terahertz light-emitting graphene-channel transistor toward single-mode lasing
title_short Terahertz light-emitting graphene-channel transistor toward single-mode lasing
title_sort terahertz light emitting graphene channel transistor toward single mode lasing
topic graphene
lasers
far infrared or terahertz
pumping
current injection
distributed-feedback
optoelectronics
url https://doi.org/10.1515/nanoph-2017-0106
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