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Güsken NA, Fu M, Zapf M, Nielsen MP, Dichtl P, Röder R, Clark AS, Maier SA, Ronning C, Oulton RF. Emission enhancement of erbium in a reverse nanofocusing waveguide. Nat Commun 2023; 14:2719. [PMID: 37169740 PMCID: PMC10175264 DOI: 10.1038/s41467-023-38262-6] [Citation(s) in RCA: 3] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/21/2022] [Accepted: 04/19/2023] [Indexed: 05/13/2023] Open
Abstract
Since Purcell's seminal report 75 years ago, electromagnetic resonators have been used to control light-matter interactions to make brighter radiation sources and unleash unprecedented control over quantum states of light and matter. Indeed, optical resonators such as microcavities and plasmonic antennas offer excellent control but only over a limited spectral range. Strategies to mutually tune and match emission and resonator frequency are often required, which is intricate and precludes the possibility of enhancing multiple transitions simultaneously. In this letter, we report a strong radiative emission rate enhancement of Er3+-ions across the telecommunications C-band in a single plasmonic waveguide based on the Purcell effect. Our gap waveguide uses a reverse nanofocusing approach to efficiently enhance, extract and guide emission from the nanoscale to a photonic waveguide while keeping plasmonic losses at a minimum. Remarkably, the large and broadband Purcell enhancement allows us to resolve Stark-split electric dipole transitions, which are typically only observed under cryogenic conditions. Simultaneous radiative emission enhancement of multiple quantum states is of great interest for photonic quantum networks and on-chip data communications.
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Affiliation(s)
- Nicholas A Güsken
- Department of Physics, Imperial College London, Prince Consort Road, London, SW7 2AZ, UK.
- Department of Materials Science and Engineering, Stanford University, Stanford, CA, 94305, USA.
| | - Ming Fu
- Department of Physics, Imperial College London, Prince Consort Road, London, SW7 2AZ, UK
| | - Maximilian Zapf
- Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743, Jena, Germany
| | - Michael P Nielsen
- Department of Physics, Imperial College London, Prince Consort Road, London, SW7 2AZ, UK
- School of Photovoltaics and Renewable Energy Engineering, UNSW Sydney, Kensington, NSW, 2052, Australia
| | - Paul Dichtl
- Department of Physics, Imperial College London, Prince Consort Road, London, SW7 2AZ, UK
| | - Robert Röder
- Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743, Jena, Germany
| | - Alex S Clark
- Department of Physics, Imperial College London, Prince Consort Road, London, SW7 2AZ, UK
- Quantum Engineering Technology Labs, University of Bristol, Bristol, BS8 1UB, UK
| | - Stefan A Maier
- Department of Physics, Imperial College London, Prince Consort Road, London, SW7 2AZ, UK
- Monash University School of Physics and Astronomy, Clayton, VIC, 3800, Australia
| | - Carsten Ronning
- Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743, Jena, Germany
| | - Rupert F Oulton
- Department of Physics, Imperial College London, Prince Consort Road, London, SW7 2AZ, UK.
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2
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Guo X, Li N, Yang X, Qi R, Wu C, Shi R, Li Y, Huang Y, García de Abajo FJ, Wang EG, Gao P, Dai Q. Hyperbolic whispering-gallery phonon polaritons in boron nitride nanotubes. NATURE NANOTECHNOLOGY 2023; 18:529-534. [PMID: 36823369 DOI: 10.1038/s41565-023-01324-3] [Citation(s) in RCA: 8] [Impact Index Per Article: 8.0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/19/2022] [Accepted: 01/11/2023] [Indexed: 05/21/2023]
Abstract
Light confinement in nanostructures produces an enhanced light-matter interaction that enables a vast range of applications including single-photon sources, nanolasers and nanosensors. In particular, nanocavity-confined polaritons display a strongly enhanced light-matter interaction in the infrared regime. This interaction could be further boosted if polaritonic modes were moulded to form whispering-gallery modes; but scattering losses within nanocavities have so far prevented their observation. Here, we show that hexagonal BN nanotubes act as an atomically smooth nanocavity that can sustain phonon-polariton whispering-gallery modes, owing to their intrinsic hyperbolic dispersion and low scattering losses. Hyperbolic whispering-gallery phonon polaritons on BN nanotubes of ~4 nm radius (sidewall of six atomic layers) are characterized by an ultrasmall nanocavity mode volume (Vm ≈ 10-10λ03 at an optical wavelength λ0 ≈ 6.4 μm) and a Purcell factor (Q/Vm) as high as 1012. We posit that BN nanotubes could become an important material platform for the realization of one-dimensional, ultrastrong light-matter interactions, with exciting implications for compact photonic devices.
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Affiliation(s)
- Xiangdong Guo
- CAS Key Laboratory of Nanophotonic Materials and Devices, CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
| | - Ning Li
- International Center for Quantum Materials, Electron Microscopy Laboratory, School of Physics, Academy for Advanced Interdisciplinary Studies, Interdisciplinary Institute of Light-Element Quantum Materials and Research Center for Light-Element Advanced Materials, Peking University, Beijing, China
| | - Xiaoxia Yang
- CAS Key Laboratory of Nanophotonic Materials and Devices, CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing, China.
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China.
| | - Ruishi Qi
- International Center for Quantum Materials, Electron Microscopy Laboratory, School of Physics, Academy for Advanced Interdisciplinary Studies, Interdisciplinary Institute of Light-Element Quantum Materials and Research Center for Light-Element Advanced Materials, Peking University, Beijing, China
| | - Chenchen Wu
- CAS Key Laboratory of Nanophotonic Materials and Devices, CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing, China
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
| | - Ruochen Shi
- International Center for Quantum Materials, Electron Microscopy Laboratory, School of Physics, Academy for Advanced Interdisciplinary Studies, Interdisciplinary Institute of Light-Element Quantum Materials and Research Center for Light-Element Advanced Materials, Peking University, Beijing, China
| | - Yuehui Li
- International Center for Quantum Materials, Electron Microscopy Laboratory, School of Physics, Academy for Advanced Interdisciplinary Studies, Interdisciplinary Institute of Light-Element Quantum Materials and Research Center for Light-Element Advanced Materials, Peking University, Beijing, China
| | - Yang Huang
- School of Materials Science and Engineering, Hebei Key Laboratory of Boron Nitride Micro and Nano Materials, Hebei University of Technology, Tianjin, China
| | - F Javier García de Abajo
- ICFO-Institut de Ciencies Fotoniques, The Barcelona Institute of Science and Technology, Castelldefels (Barcelona), Spain.
- ICREA-Institució Catalana de Recerca i Estudis Avançats, Barcelona, Spain.
| | - En-Ge Wang
- Collaborative Innovation Center of Quantum Matter, Beijing, China
- Songshan Lake Materials Lab, Institute of Physics, Chinese Academy of Sciences, Guangdong, China
- School of Physics, Liaoning University, Shenyang, China
| | - Peng Gao
- International Center for Quantum Materials, Electron Microscopy Laboratory, School of Physics, Academy for Advanced Interdisciplinary Studies, Interdisciplinary Institute of Light-Element Quantum Materials and Research Center for Light-Element Advanced Materials, Peking University, Beijing, China.
- Collaborative Innovation Center of Quantum Matter, Beijing, China.
| | - Qing Dai
- CAS Key Laboratory of Nanophotonic Materials and Devices, CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center for Excellence in Nanoscience, National Center for Nanoscience and Technology, Beijing, China.
- Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China.
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3
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Kang L, Fei H, Lin H, Wu M, Wang X, Zhang M, Liu X, Sun F, Chen Z. Thermal tunable silicon valley photonic crystal ring resonators at the telecommunication wavelength. OPTICS EXPRESS 2023; 31:2807-2815. [PMID: 36785286 DOI: 10.1364/oe.475559] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/15/2022] [Accepted: 11/21/2022] [Indexed: 06/18/2023]
Abstract
Tunable ring resonators are essential devices in integrated circuits. Compared to conventional ring resonators, valley photonic crystal (VPC) ring resonators have a compact design and high quality factor (Q-factor), attracting broad attention. However, tunable VPC ring resonators haven't been demonstrated. Here we theoretically demonstrate the first tunable VPC ring resonator in the telecommunication wavelength region, the resonance peaks of which are tuned by controlling the temperature based on the thermal-optic effect of silicon. The design is ultracompact (12.05 µm by 10.44 µm), with a high Q-factor of 1281.00. By tuning the temperature from 100 K to 750 K, the phase modulation can reach 7.70 π, and the adjustment efficiency is 0.062 nm/K. Since thermal tuning has been broadly applied in silicon photonics, our design can be readily applied in integrated photonic circuits and will find broad applications. Furthermore, our work opens new possibilities and deepens the understanding of designing novel tunable VPC photonic devices.
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Moeinimaleki B, Kaatuzian H, Livani AM. Design and simulation of a plasmonic density nanosensor for polarizable gases. APPLIED OPTICS 2022; 61:4735-4742. [PMID: 36255954 DOI: 10.1364/ao.457454] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/03/2022] [Accepted: 04/22/2022] [Indexed: 06/16/2023]
Abstract
In this paper, an optical method of measuring the mass density of polarizable gases is proposed using a plasmonic refractive index nano-sensor. Plasmonic sensors can detect very small changes in the refracting index of arbitrary dielectric materials. However, attributing them to a specific application needs more elaboration of the material's refractive index unit's (RIU) relation with the introduced application. In a gaseous medium, the optical properties of molecules are related to their dipole moment polarizability. Hence, the theoretical index-density relation of Lorentz-Lorenz is applied in the proposed sensing mechanism to interpret changes in the gas' refractive index and to changes in its density. The proposed plasmonic mass density sensor shows a sensitivity of 348.8nm/(gr/cm3) for methane gas in the visible light region. This sensor can be integrated with photonic circuits for gas sensing purposes.
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Huang CC, Chang RJ, Huang CC. Nanostructured hybrid plasmonic waveguide in a slot structure for high-performance light transmission. OPTICS EXPRESS 2021; 29:29341-29356. [PMID: 34615045 DOI: 10.1364/oe.438771] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/26/2021] [Accepted: 08/17/2021] [Indexed: 06/13/2023]
Abstract
Squeezing light to nanoscale is the most vital capacity of nanophotonic circuits processing on-chip optical signals that allows to significantly enhance light-matter interaction by stimulating various nonlinear optical effects. It is well known that plasmon can offer an unrivaled concentration of optical energy beyond the optical diffraction limit. However, the progress of plasmonic technology is mainly hindered by its ohmic losses, thus leading to the difficulty in building large-area photonic integrated circuits. To significantly increase the propagation distance of light, we develop a new waveguide structure operating at the telecommunication wavelength of 1,550 nm. It consists of a nanostructured hybrid plasmonic waveguide embedded in a high-index-contrast slot waveguide. We capitalize on the strong mode confinement of the slot waveguide and reduce mode areas with the nanostructured hybrid plasmonic configuration while maintaining extremely low ohmic losses using a nanoscale metal strip. The proposed design achieves a record propagation distance of 1,115 µm while comparing with that of other designs at a mode area of the order of 10-5A0 (A0 is the diffraction-limited area). The mode characterization considering fabrication imperfections and spectral responses show the robustness and broadband operation range of the proposed waveguide. Moreover, we also investigated the crosstalk to assess the density of integration. The proposed design paves the way for building nanophotonic circuits and optoelectronic devices that require strong light-matter interaction.
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Ren T, Dong Y, Xu S, Gong X. Strong Purcell effect in deep subwavelength coaxial cavity with GeSn active medium. OPTICS LETTERS 2021; 46:3889-3892. [PMID: 34388767 DOI: 10.1364/ol.432164] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/21/2021] [Accepted: 06/30/2021] [Indexed: 06/13/2023]
Abstract
We propose a deep subwavelength plasmonic cavity based on a metal-coated coaxial structure with Ge0.9Sn0.1 as the active medium. A fundamental surface plasmon polariton mode is strongly confined on the sidewall of the metal core, with the quality factor up to 5×103 at 10 K. By reducing the cavity dimension to a few nanometers, this cavity mode shows a strong plasmon binding with the mode volume down to 8×10-10 (λ/n)3, and significant size-dependent damping caused by the non-local optical response. The Purcell factor is achieved as high as 2×109 at 10 K and 7×108 at 300 K. This cavity design provides a systematic guideline of scaling down the cavity size and enhancing the Purcell factor. Our theoretical demonstration and understanding of the subwavelength plasmonic cavity represent a significant step toward the large-scale integration of on-chip lasers with a low threshold.
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Huang Q, Jia J, Forsberg E, He S. LiNbO 3 waveguide with embedded Ag nanowire and 3L MoS 2 for strong light confinement and ultra-long propagation length in the visible spectral range. OPTICS EXPRESS 2021; 29:7168-7178. [PMID: 33726223 DOI: 10.1364/oe.418907] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/08/2021] [Accepted: 02/17/2021] [Indexed: 06/12/2023]
Abstract
A vertical slot LiNbO3 waveguide with an Ag nanowire and 3L MoS2 embedded in the low-refractive index slot region is proposed for the purpose of improving light confinement. We find that the proposed waveguide has a novel dielectric based plasmonic mode, where local light field is enhanced by the Ag nanowire. The mode exhibits an extremely large figure of merit (FoM) of 6.5×106, one order of magnitude larger than that the largest FoM of any plasmonic waveguide reported in the literature to date. The waveguide also has an extremely long propagation length of 84 cm in the visible wavelength at 680 nm. Furthermore, the waveguide has a low sub-micro bending loss and can be directly connected to all-dielectric waveguides with an extremely low coupling loss. The proposed vertical slot LiNbO3 waveguide is a promising candidate for the realization of ultrahigh integration density tunable circuits in the visible spectral range.
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Lin CCC, Chang PH, Helmy AS. Supermode Hybridization: A Material-Independent Route toward Record Schottky Detection Sensitivity Using <0.05 μm 3 Amorphous Absorber Volume. NANO LETTERS 2020; 20:8500-8507. [PMID: 33231473 DOI: 10.1021/acs.nanolett.0c02831] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/11/2023]
Abstract
Schottky photodetectors are attractive for CMOS-compatible photonic integrated circuits, but the inability to simultaneously optimize the metal emitter thickness for photon absorption and hot carrier emission limits the detection efficiency and sensitivity. Here, we propose and experimentally demonstrate a supermode hybridization waveguiding effect that can overcome the trade-off. By introducing structural asymmetry into coupled plasmonic nanostructures, hybridization-induced field enhancement can help ultrathin metal emitters to achieve greater optical absorption than bulk counterparts. Despite the use of amorphous materials with higher transport losses, our hybridized Schottky detectors demonstrate higher responsivity per device volume compared to crystalline-based and unhybridized Schottky designs with broadband (1.5-1.6 μm) and athermal (15-100 °C) behavior as well as record sensitivity of -55 dBm that approaches Ge counterparts that are 36 times larger. The hybridization effect can be utilized across diverse nanomaterial platforms to facilitate light-matter interaction, paving the way toward backend-compatible, chip-integrated photonics with greater manufacturing flexibility.
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Affiliation(s)
- Charles Chih-Chin Lin
- The Edward S. Rogers Department of Electrical and Computer Engineering, University of Toronto, 10 King's College Road, Toronto, Ontario M5S 3G4, Canada
| | - Po-Han Chang
- The Edward S. Rogers Department of Electrical and Computer Engineering, University of Toronto, 10 King's College Road, Toronto, Ontario M5S 3G4, Canada
| | - Amr S Helmy
- The Edward S. Rogers Department of Electrical and Computer Engineering, University of Toronto, 10 King's College Road, Toronto, Ontario M5S 3G4, Canada
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9
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Shang Q, Li M, Zhao L, Chen D, Zhang S, Chen S, Gao P, Shen C, Xing J, Xing G, Shen B, Liu X, Zhang Q. Role of the Exciton-Polariton in a Continuous-Wave Optically Pumped CsPbBr 3 Perovskite Laser. NANO LETTERS 2020; 20:6636-6643. [PMID: 32786951 DOI: 10.1021/acs.nanolett.0c02462] [Citation(s) in RCA: 59] [Impact Index Per Article: 14.8] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/22/2023]
Abstract
Lead halide perovskites have emerged as excellent optical gain materials for solution-processable and flexible lasers. Recently, continuous-wave (CW) optically driven lasing was established in perovskite crystals; however, the mechanism of low-threshold operation is still disputed. In this study, CW-pumped lasing from one-dimensional CsPbBr3 nanoribbons (NBs) with a threshold of ∼130 W cm-2 is demonstrated, which can be ascribed to the large refractive index induced by the exciton-polariton (EP) effect. Increasing the temperature reduces the exciton fraction of EPs, which decreases the group and phase refractive indices and inhibits lasing above 100 K. Thermal management, including reducing the NB height to ∼120 ± 60 nm and adopting a high-thermal-conductivity sink, e.g., sapphire, is critical for CW-driven lasing, even at cryogenic temperatures. These results reveal the nature of ultralow-threshold lasing with CsPbBr3 and provide insights into the construction of room-temperature CW and electrically driven perovskite macro/microlasers.
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Affiliation(s)
- Qiuyu Shang
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
| | - Meili Li
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
| | - Liyun Zhao
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
| | - Dingwei Chen
- State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
| | - Shuai Zhang
- CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center of Excellence for Nanoscience, National Center for Nanoscience and Technology, Beijing 100190, China
| | - Shulin Chen
- School of Physics, Peking University, Beijing 100871, China
- Electron Microscopy Laboratory, International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
| | - Peng Gao
- School of Physics, Peking University, Beijing 100871, China
- Electron Microscopy Laboratory, International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China
| | - Chao Shen
- State Key Laboratory of Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
| | - Jun Xing
- Key Laboratory of Eco-Chemical Engineering, Ministry of Education, College of Chemistry and Molecular Engineering, Qingdao University of Science and Technology, Qingdao 266042, China
| | - Guichuan Xing
- Joint Key Laboratory of the Ministry of Education, Institute of Applied Physics and Materials Engineering, University of Macau, Avenida da Universidade Taipa, Macao 999078, China
| | - Bo Shen
- School of Physics, Peking University, Beijing 100871, China
- Research Center for Wide Gap Semiconductor, Peking University, Beijing 100871, China
| | - Xinfeng Liu
- CAS Key Laboratory of Standardization and Measurement for Nanotechnology, CAS Center of Excellence for Nanoscience, National Center for Nanoscience and Technology, Beijing 100190, China
| | - Qing Zhang
- Department of Materials Science and Engineering, College of Engineering, Peking University, Beijing 100871, China
- Research Center for Wide Gap Semiconductor, Peking University, Beijing 100871, China
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Lin CCC, Chang PH, Su Y, Helmy AS. Monolithic Plasmonic Waveguide Architecture for Passive and Active Optical Circuits. NANO LETTERS 2020; 20:2950-2957. [PMID: 32227898 DOI: 10.1021/acs.nanolett.9b04612] [Citation(s) in RCA: 8] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/10/2023]
Abstract
Guided-wave plasmonic circuits are promising platforms for sensing, interconnection, and quantum applications in the subdiffraction regime. Nonetheless, the loss-confinement trade-off remains a collective bottleneck for plasmonic-enhanced optical processes. Here, we report a unique plasmonic waveguide architecture that can alleviate such trade-off and improve the efficiencies of plasmonic-based emission, light-matter-interaction, and detection simultaneously. Specifically, record experimental attributes such as normalized Purcell factor approaching 104, 10 dB amplitude modulation with <1 dB insertion loss and fJ-level switching energy, and photodetection sensitivity and internal quantum efficiency of -54 dBm and 6.4% respectively have been realized within our amorphous-based, coupled-mode plasmonic structure. The ability to support multiple optoelectronic phenomena while providing performance gains over existing plasmonic and dielectric counterparts offers a clear path toward reconfigurable, monolithic plasmonic circuits.
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Affiliation(s)
- Charles Chih-Chin Lin
- Department of Electrical and Computer Engineering, University of Toronto, Ontario, Canada
| | - Po-Han Chang
- Department of Electrical and Computer Engineering, University of Toronto, Ontario, Canada
| | - Yiwen Su
- Department of Electrical and Computer Engineering, University of Toronto, Ontario, Canada
| | - Amr S Helmy
- Department of Electrical and Computer Engineering, University of Toronto, Ontario, Canada
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Voronin KV, Stebunov YV, Voronov AA, Arsenin AV, Volkov VS. Vertically Coupled Plasmonic Racetrack Ring Resonator for Biosensor Applications. SENSORS 2019; 20:s20010203. [PMID: 31905897 PMCID: PMC6983217 DOI: 10.3390/s20010203] [Citation(s) in RCA: 11] [Impact Index Per Article: 2.2] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 12/01/2019] [Revised: 12/23/2019] [Accepted: 12/26/2019] [Indexed: 02/04/2023]
Abstract
Plasmonic chemical and biological sensors offer significant advantages such as really compact sizes and extremely high sensitivity. Biosensors based on plasmonic waveguides and resonators are some of the most attractive candidates for mobile and wearable devices. However, high losses in the metal and complicated schemes for practical implementation make it challenging to find the optimal configuration of a compact plasmon biosensor. Here, we propose a novel plasmonic refractive index sensor based on a metal strip waveguide placed under a waveguide-based racetrack ring resonator made of the same metal. This scheme guarantees effective coupling between the waveguide and resonator and low loss light transmittance through the long-range waveguide. The proposed device can be easily fabricated (e.g., using optical lithography) and integrated with materials like graphene oxide for providing adsorption of the biomolecules on the sensitive part of the optical elements. To analyze the properties of the designed sensing system, we performed numerical simulations along with some analytical estimations. There is one other interesting general feature of this sensing scheme that is worth pointing out before looking at its details. The sensitivity of the considered device can be significantly increased by surrounding the resonator with media of slightly different refractive indices, which allows sensitivity to reach a value of more than 1 μm per refractive index unit.
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Affiliation(s)
- Kirill V. Voronin
- Center for Photonics & 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia; (K.V.V.); (Y.V.S.); (A.A.V.); (A.V.A.)
- Skolkovo Institute of Science and Technology, Bolshoy Boulevard 30, bld. 1, Moscow 121205, Russia
| | - Yury V. Stebunov
- Center for Photonics & 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia; (K.V.V.); (Y.V.S.); (A.A.V.); (A.V.A.)
- GrapheneTek, 7 Nobel Street, Skolkovo Innovation Center, Moscow 143026, Russia
| | - Artem A. Voronov
- Center for Photonics & 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia; (K.V.V.); (Y.V.S.); (A.A.V.); (A.V.A.)
| | - Aleksey V. Arsenin
- Center for Photonics & 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia; (K.V.V.); (Y.V.S.); (A.A.V.); (A.V.A.)
- GrapheneTek, 7 Nobel Street, Skolkovo Innovation Center, Moscow 143026, Russia
| | - Valentyn S. Volkov
- Center for Photonics & 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia; (K.V.V.); (Y.V.S.); (A.A.V.); (A.V.A.)
- GrapheneTek, 7 Nobel Street, Skolkovo Innovation Center, Moscow 143026, Russia
- Correspondence: ; Tel.: +7-926-735-9398
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