Mid-infrared active graphene nanoribbon plasmonic waveguide devices

Doped graphene emerges as a strong contender for active plasmonic material in mid-infrared wavelengths due to the versatile external control of its permittivity function and also its highly compressed graphene surface plasmon (GSP) wavelength. In this paper, we design active plasmonic waveguide devi...

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Main Authors: Ooi, Kelvin Jian Aun, Chu, Hong Son, Ang, L. K., Bai, Ping
Other Authors: School of Electrical and Electronic Engineering
Format: Article
Language:English
Published: 2016
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Online Access:https://hdl.handle.net/10356/82175
http://hdl.handle.net/10220/41139
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-821752020-03-07T13:57:28Z Mid-infrared active graphene nanoribbon plasmonic waveguide devices Ooi, Kelvin Jian Aun Chu, Hong Son Ang, L. K. Bai, Ping School of Electrical and Electronic Engineering Thin films Plasmonics Doped graphene emerges as a strong contender for active plasmonic material in mid-infrared wavelengths due to the versatile external control of its permittivity function and also its highly compressed graphene surface plasmon (GSP) wavelength. In this paper, we design active plasmonic waveguide devices based on electrical modulation of doped graphene nanoribbons (GNRs) on a voltage-gated inhomogeneous dielectric layer. We first develop figure-of-merit (FoM) formulae to characterize the performance of passive and active graphene nanoribbon waveguides. Based on the FoMs, we choose optimal GNRs to build a plasmonic shutter, which consists of a GNR placed on top of an inhomogeneous SiO2 substrate supported by a Si nanopillar. Simulation studies show that for a simple, 50 nm long plasmonic shutter, the modulation contrast can exceed 30 dB. The plasmonic shutter is further extended to build a four-port active power splitter and an eight-port active network, both based on GNR cross-junction waveguides. For the active power splitter, the GSP power transmission at each waveguide arm can be independently controlled by an applied gate voltage with high-modulation contrast and nearly equal power-splitting proportions. From the construct of the eight-port active network, we see that it is possible to scale up the GNR cross-junction waveguides into large and complex active waveguide networks, showing great potential in an exciting new area of mid-infrared graphene plasmonic integrated nanocircuits. ASTAR (Agency for Sci., Tech. and Research, S’pore) MOE (Min. of Education, S’pore) 2016-08-16T08:22:04Z 2019-12-06T14:48:01Z 2016-08-16T08:22:04Z 2019-12-06T14:48:01Z 2013 Journal Article Ooi, K. J. A., Chu, H. S., Ang, L. K., & Bai, P. (2013). Mid-infrared active graphene nanoribbon plasmonic waveguide devices. Journal of the Optical Society of America B, 30(12), 3111-3116. 0740-3224 https://hdl.handle.net/10356/82175 http://hdl.handle.net/10220/41139 10.1364/JOSAB.30.003111 en Journal of the Optical Society of America B © 2013 Optical Society of America.
institution Nanyang Technological University
building NTU Library
country Singapore
collection DR-NTU
language English
topic Thin films
Plasmonics
spellingShingle Thin films
Plasmonics
Ooi, Kelvin Jian Aun
Chu, Hong Son
Ang, L. K.
Bai, Ping
Mid-infrared active graphene nanoribbon plasmonic waveguide devices
description Doped graphene emerges as a strong contender for active plasmonic material in mid-infrared wavelengths due to the versatile external control of its permittivity function and also its highly compressed graphene surface plasmon (GSP) wavelength. In this paper, we design active plasmonic waveguide devices based on electrical modulation of doped graphene nanoribbons (GNRs) on a voltage-gated inhomogeneous dielectric layer. We first develop figure-of-merit (FoM) formulae to characterize the performance of passive and active graphene nanoribbon waveguides. Based on the FoMs, we choose optimal GNRs to build a plasmonic shutter, which consists of a GNR placed on top of an inhomogeneous SiO2 substrate supported by a Si nanopillar. Simulation studies show that for a simple, 50 nm long plasmonic shutter, the modulation contrast can exceed 30 dB. The plasmonic shutter is further extended to build a four-port active power splitter and an eight-port active network, both based on GNR cross-junction waveguides. For the active power splitter, the GSP power transmission at each waveguide arm can be independently controlled by an applied gate voltage with high-modulation contrast and nearly equal power-splitting proportions. From the construct of the eight-port active network, we see that it is possible to scale up the GNR cross-junction waveguides into large and complex active waveguide networks, showing great potential in an exciting new area of mid-infrared graphene plasmonic integrated nanocircuits.
author2 School of Electrical and Electronic Engineering
author_facet School of Electrical and Electronic Engineering
Ooi, Kelvin Jian Aun
Chu, Hong Son
Ang, L. K.
Bai, Ping
format Article
author Ooi, Kelvin Jian Aun
Chu, Hong Son
Ang, L. K.
Bai, Ping
author_sort Ooi, Kelvin Jian Aun
title Mid-infrared active graphene nanoribbon plasmonic waveguide devices
title_short Mid-infrared active graphene nanoribbon plasmonic waveguide devices
title_full Mid-infrared active graphene nanoribbon plasmonic waveguide devices
title_fullStr Mid-infrared active graphene nanoribbon plasmonic waveguide devices
title_full_unstemmed Mid-infrared active graphene nanoribbon plasmonic waveguide devices
title_sort mid-infrared active graphene nanoribbon plasmonic waveguide devices
publishDate 2016
url https://hdl.handle.net/10356/82175
http://hdl.handle.net/10220/41139
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