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Kulikova DP, Sgibnev YM, Yankovskii GM, Chubchev ED, Lotkov ES, Ezenkova DA, Dobronosova AA, Baburin AS, Rodionov IA, Nechepurenko IA, Baryshev AV, Dorofeenko AV. Optical hydrogen sensing with high-Q guided-mode resonance of Al 2O 3/WO 3/Pd nanostructure. Sci Rep 2023; 13:890. [PMID: 36650224 PMCID: PMC9845354 DOI: 10.1038/s41598-023-28204-z] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/24/2022] [Accepted: 01/13/2023] [Indexed: 01/18/2023] Open
Abstract
Nanostructure based on a dielectric grating (Al2O3), gasochromic oxide (WO3) and catalyst (Pd) is proposed as a hydrogen sensor working at the room temperature. In the fabricated structure, the Pd catalyst film was as thin as 1 nm that allowed a significant decrease in the optical absorption. A high-Q guided-mode resonance was observed in a transmission spectrum at normal incidence and was utilized for hydrogen detection. The spectra were measured at 0-0.12% of hydrogen in a synthetic air (≈ 80% [Formula: see text] and 20% [Formula: see text]). The detection limit below 100 ppm of hydrogen was demonstrated. Hydrogen was detected in the presence of oxygen, which provides the sensor recovery but suppresses the sensor response. Sensor response was treated by the principal component analysis (PCA), which effectively performs noise averaging. Influence of temperature and humidity was measured and processed by PCA, and elimination of the humidity and temperature effects was performed. Square root dependence of the sensor response on the hydrogen concentration (Sievert's law) was observed. Sensor calibration curve was built, and the sensor resolution of 40 ppm was found. Long term stability of the sensor was investigated. Particularly, it was shown that the sensor retains its functionality after 6 months and dozens of acts of response to gas.
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Affiliation(s)
- Daria P. Kulikova
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.14476.300000 0001 2342 9668Faculty of Physics, Lomonosov Moscow State University, Moscow, Russia
| | - Yevgeniy M. Sgibnev
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia
| | - Georgiy M. Yankovskii
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia
| | - Eugeny D. Chubchev
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia
| | - Evgeniy S. Lotkov
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.61569.3d0000 0001 0405 5955FMN Laboratory, Bauman Moscow State Technical University, Moscow, Russia
| | - Daria A. Ezenkova
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.61569.3d0000 0001 0405 5955FMN Laboratory, Bauman Moscow State Technical University, Moscow, Russia
| | - Alina A. Dobronosova
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.61569.3d0000 0001 0405 5955FMN Laboratory, Bauman Moscow State Technical University, Moscow, Russia
| | - Aleksandr S. Baburin
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.61569.3d0000 0001 0405 5955FMN Laboratory, Bauman Moscow State Technical University, Moscow, Russia
| | - Ilya A. Rodionov
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.61569.3d0000 0001 0405 5955FMN Laboratory, Bauman Moscow State Technical University, Moscow, Russia
| | - Igor A. Nechepurenko
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.4886.20000 0001 2192 9124Kotelnikov Institute of Radioengineering and Electronics RAS, Moscow, Russia ,grid.18763.3b0000000092721542Moscow Institute of Physics and Technology, Dolgoprudny, Moscow, Russia
| | - Alexander V. Baryshev
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia
| | - Alexander V. Dorofeenko
- grid.472660.10000 0004 0544 1518Dukhov Research Institute of Automatics (VNIIA), Moscow, Russia ,grid.18763.3b0000000092721542Moscow Institute of Physics and Technology, Dolgoprudny, Moscow, Russia ,grid.473298.3Institute for Theoretical and Applied Electromagnetics RAS, Moscow, Russia
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Reshetnyak VY, Pinkevych IP, Bunning TJ, McConney ME, Evans DR. Spectral manifestation of optical Tamm states in a metal-cholesteric liquid crystals stack. Phys Rev E 2023; 107:014702. [PMID: 36797897 DOI: 10.1103/physreve.107.014702] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/14/2022] [Accepted: 01/08/2023] [Indexed: 06/18/2023]
Abstract
The reflection spectrum of linearly polarized light by a system consisting of a metal film and two adjacent sequentially located cholesteric liquid crystals (CLCs) with opposite helical twists is theoretically studied. The system contains a dielectric index-matching layer (DIML) between the metal film and the CLC layers. It is shown that in such a system the excitation of optical Tamm states (OTSs) by linearly polarized light is possible. The influence of the CLC pitch, refractive indices, and thicknesses of the DIML and metal film on the OTS manifestation in the reflection spectrum of the system is studied. The strong influence of the DIML thickness on the OTS wavelength and the appearance of multiple OTSs with an increase in the DIML thickness is noted.
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Affiliation(s)
- V Yu Reshetnyak
- Physics Faculty, Taras Shevchenko National University of Kyiv, 64 Volodymyrs'ka Street, Kyiv 01601, Ukraine
- School of Physics and Astronomy, University of Leeds, Leeds LS2 9JT, United Kingdom
| | - I P Pinkevych
- Physics Faculty, Taras Shevchenko National University of Kyiv, 64 Volodymyrs'ka Street, Kyiv 01601, Ukraine
| | - T J Bunning
- Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson Air Force Base, Dayton 45433, USA
| | - M E McConney
- Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson Air Force Base, Dayton 45433, USA
| | - D R Evans
- Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson Air Force Base, Dayton 45433, USA
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Reshetnyak VY, Pinkevych IP, Bunning TJ, Evans DR. Influence of Rugate Filters on the Spectral Manifestation of Tamm Plasmon Polaritons. MATERIALS 2021; 14:ma14051282. [PMID: 33800265 PMCID: PMC7962660 DOI: 10.3390/ma14051282] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 02/13/2021] [Revised: 03/02/2021] [Accepted: 03/04/2021] [Indexed: 11/30/2022]
Abstract
This study theoretically investigated light reflection and transmission in a system composed of a thin metal layer (Ag) adjacent to a rugate filter (RF) having a harmonic refractive index profile. Narrow dips in reflectance and peaks in transmittance in the RF band gap were obtained due to the excitation of a Tamm plasmon polariton (TPP) at the Ag–RF interface. It is shown that the spectral position and magnitude of the TPP dips/peaks in the RF band gap depend on the harmonic profile parameters of the RF refractive index, the metal layer thickness, and the external medium refractive index. The obtained dependences for reflectance and transmittance allow selecting parameters of the system which can be optimized for various applications.
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Affiliation(s)
| | - Igor P. Pinkevych
- Physics Faculty, Taras Shevchenko National University of Kyiv, 01601 Kyiv, Ukraine;
- Correspondence:
| | - Timothy J. Bunning
- Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson Air Force Base, OH 45433, USA
| | - Dean R. Evans
- Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson Air Force Base, OH 45433, USA
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Control of the surface plasmon dispersion and Purcell effect at the metamaterial-dielectric interface. Sci Rep 2020; 10:20828. [PMID: 33257765 PMCID: PMC7705705 DOI: 10.1038/s41598-020-77688-6] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/09/2020] [Accepted: 10/16/2020] [Indexed: 11/09/2022] Open
Abstract
The use of metamaterial as a way to mitigate the negative effects of absorption in metals on the Purcell effect in metal-dielectric structures is investigated. A layered metal-dielectric structure is considered as an anisotropic medium in the long-wavelength limit. The dispersion of the surface plasmon appearing at the boundary between such a structure and a different dielectric material, as well as the position of the peak in the local density of states are studied for various combinations of materials and filling factors of the periodic structure. The calculated frequency dependence of the Purcell factor demonstrates an increase in peak value compared to the conventional plasmonic structure. The results obtained using effective media approach are compared to the results of numerical modelling.
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Revising of the Purcell effect in periodic metal-dielectric structures: the role of absorption. Sci Rep 2019; 9:9604. [PMID: 31270385 PMCID: PMC6610144 DOI: 10.1038/s41598-019-46071-5] [Citation(s) in RCA: 14] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/30/2019] [Accepted: 06/18/2019] [Indexed: 11/10/2022] Open
Abstract
Periodic metal-dielectric structures attract substantial interest since it was previously proposed that the spontaneous emission amplification rates (the Purcell factor) in such structures can reach enormous values up to 105. However, the role of absorption in real metals has not been thoroughly considered. We provide a theoretical analysis showing that absorption leads to diminishing values of Purcell factor. We also suggest that using emitting organic compounds such as CBP (4,4-Bis(N-carbazolyl)-1,1-biphenyl) can lead to a moderate increase of about an order of magnitude in the Purcell factor. Defining the experimentally measured Purcell factor as a ratio between the excited state lifetimes in bare CBP and in periodic structure, this increase in the fabricated periodic structure is demonstrated through a 4–8 times decrease in excited state radiative lifetime compared to a bare organic material in a wide emission spectrum.
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Ge D, Shi J, Rezk A, Zhang Y, Wei J, Zhang L, Zhu S. Optical Fano resonance sensing of bilayer asymmetric photonic crystal slabs as biosensors. APPLIED OPTICS 2019; 58:3187-3192. [PMID: 31044793 DOI: 10.1364/ao.58.003187] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/26/2018] [Accepted: 03/25/2019] [Indexed: 05/20/2023]
Abstract
A bilayer asymmetric photonic crystal slab made of porous Si3N4/SiO2 is designed as a biosensor by considering the optical performance of this photonic crystal slab with a square lattice based on rigorous coupled-wave analysis theory and wavelength interrogation methods. The results show that this bilayer asymmetric photonic crystal can be used as a biosensor according to its excellent linearity relationship between the guided resonance peak shift and refractive index of aqueous solution with or without glycerol. The theoretical sensitivity value of the bilayer asymmetric photonic crystal biosensor is achieved as (S>286 nm/RIU) in the wavelength range from 1400 nm to 1600 nm. These results also indicate that the asymmetry bilayer structure has an important influence on its optical characteristic and sensitivity of the bilayer photonic crystal biosensor, and hence, it can be modified by changing the lattice constant and slab thickness. This research paper is very useful for understanding the application and design of biosensors based on porous structures.
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Abstract
The paper has proposed a new structure based on MoS2. The electric field distribution, the locality and the loss of the mode, and the threshold under different geometric shapes and parameters are investigated using COMSOL Multiphysics software, based on the finite element method. The different influenced degree of each component is also analyzed. Simulation results reveal that this kind of nanolaser has a low loss and high field confinement ability, the radius of CdS and Ag make a major contribution to the low loss and low threshold, and field confinement ability is mainly affected by the height of air gap. Under optimal parameters, effective propagation loss is only 0.00013, and the lasing threshold can be as low as 0.11 μm−1. The results provide theory and technique support to the field of new nanolaser design.
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Bloch-Surface-Polariton-Based Hybrid Nanowire Structure for Subwavelength, Low-Loss Waveguiding. APPLIED SCIENCES-BASEL 2018. [DOI: 10.3390/app8030358] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/17/2022]
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Gubaydullin AR, Symonds C, Bellessa J, Ivanov KA, Kolykhalova ED, Sasin ME, Lemaitre A, Senellart P, Pozina G, Kaliteevski MA. Enhancement of spontaneous emission in Tamm plasmon structures. Sci Rep 2017; 7:9014. [PMID: 28827784 PMCID: PMC5567056 DOI: 10.1038/s41598-017-09245-7] [Citation(s) in RCA: 49] [Impact Index Per Article: 6.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/16/2016] [Accepted: 07/25/2017] [Indexed: 11/09/2022] Open
Abstract
It was theoretically and experimentally demonstrated that in metal/semiconductor Tamm plasmon structures the probability of spontaneous emission can be increased despite losses in metal, and theoretical analysis of experimental results suggested that the enhancement could be as high as one order of magnitude. Tamm plasmon structure with quantum dots has been fabricated and the emission pattern has been measured. Electromagnetic modes of the structure have been analyzed and modification of spontaneous emission rates has been calculated showing a good agreement with experimentally observed emission pattern.
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Affiliation(s)
- A R Gubaydullin
- St Petersburg Academic University, 8/3 Khlopina Str, St Petersburg, 194021, Russia.,Univ Lyon, Université Claude Bernard Lyon 1, CNRS, Institut Lumière Matière, F-69622, LYON, France
| | - C Symonds
- Univ Lyon, Université Claude Bernard Lyon 1, CNRS, Institut Lumière Matière, F-69622, LYON, France
| | - J Bellessa
- Univ Lyon, Université Claude Bernard Lyon 1, CNRS, Institut Lumière Matière, F-69622, LYON, France
| | - K A Ivanov
- St Petersburg Academic University, 8/3 Khlopina Str, St Petersburg, 194021, Russia.,ITMO University, 49 Kronverksky Pr., St. Petersburg, 197101, Russia
| | - E D Kolykhalova
- St Petersburg Academic University, 8/3 Khlopina Str, St Petersburg, 194021, Russia.,Ioffe Institute, 26 Politekhnicheskaya, St. Petersburg, 194021, Russian Federation
| | - M E Sasin
- Ioffe Institute, 26 Politekhnicheskaya, St. Petersburg, 194021, Russian Federation
| | - A Lemaitre
- Centre de Nanosciences et Nanotechnologies, CNRS Université Paris-Saclay, Route de Nozay, F-91460, Marcoussis, France
| | - P Senellart
- Centre de Nanosciences et Nanotechnologies, CNRS Université Paris-Saclay, Route de Nozay, F-91460, Marcoussis, France
| | - G Pozina
- Department of Physics, Chemistry and Biology, Linköping University, 58183, Linköping, Sweden.
| | - M A Kaliteevski
- St Petersburg Academic University, 8/3 Khlopina Str, St Petersburg, 194021, Russia.,ITMO University, 49 Kronverksky Pr., St. Petersburg, 197101, Russia.,Ioffe Institute, 26 Politekhnicheskaya, St. Petersburg, 194021, Russian Federation
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Plasmonic Photonic-Crystal Slabs: Visualization of the Bloch Surface Wave Resonance for an Ultrasensitive, Robust and Reusable Optical Biosensor. CRYSTALS 2014. [DOI: 10.3390/cryst4040498] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
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