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1

Buchnev, Oleksandr, Alexandr Belosludtsev, Victor Reshetnyak, Dean R. Evans, and Vassili A. Fedotov. "Observing and controlling a Tamm plasmon at the interface with a metasurface." Nanophotonics 9, no. 4 (March 18, 2020): 897–903. http://dx.doi.org/10.1515/nanoph-2019-0514.

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AbstractWe demonstrate experimentally that Tamm plasmons in the near infrared can be supported by a dielectric mirror interfaced with a metasurface, a discontinuous thin metal film periodically patterned on the sub-wavelength scale. More crucially, not only do Tamm plasmons survive the nanopatterning of the metal film but they also become sensitive to external perturbations as a result. In particular, by depositing a nematic liquid crystal on the outer side of the metasurface, we were able to red shift the spectral position of Tamm plasmon by 35 nm, while electrical switching of the liquid crystal enabled us to tune the wavelength of this notoriously inert excitation within a 10-nm range.
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2

Balevičius, Zigmas. "Strong Coupling between Tamm and Surface Plasmons for Advanced Optical Bio-Sensing." Coatings 10, no. 12 (December 5, 2020): 1187. http://dx.doi.org/10.3390/coatings10121187.

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The total internal reflection ellipsometry method was used to analyse the angular spectra of the hybrid Tamm and surface plasmon modes and to compare their results with those obtained using the conventional single SPR method. As such type of measurement is quite common in commercial SPR devices, more detailed attention was paid to the analysis of the p-polarization reflection intensity dependence. The conducted study showed that the presence of strong coupling in the hybrid plasmonic modes increases the sensitivity of the plasmonic-based sensors due to the reduced losses in the metal layer. The experimental results and analysis of the optical responses of three different plasmonic-based samples indicated that the optimized Tamm plasmons ΔRp(TP) and optimized surface plasmons ΔRp(SP) samples produce a response that is about five and six times greater than the conventional surface plasmon resonance ΔRp(SPR) in angular spectra. The sensitivity of the refractive index unit of the spectroscopic measurements for the optimized Tamm plasmon samples was 1.5 times higher than for conventional SPR, while for wavelength scanning, the SPR overcame the optimized TP by 1.5 times.
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3

Bikbaev, Rashid, Stepan Vetrov, and Ivan Timofeev. "Epsilon-Near-Zero Absorber by Tamm Plasmon Polariton." Photonics 6, no. 1 (March 9, 2019): 28. http://dx.doi.org/10.3390/photonics6010028.

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Two schemes of excitation of a Tamm plasmon polariton localized at the interface between a photonic crystal and a nanocomposite with near-zero effective permittivity have been investigated in the framework of the temporal coupled-mode theory. The parameters of the structure have been determined, which correspond to the critical coupling of the incident field with a Tamm plasmon polariton and, consequently, ensure the total absorption of the incident radiation by the structure. It has been established that the spectral width of the absorption line depends on the scheme of Tamm plasmon polariton excitation and the parameters of a nanocomposite film. The features of field localization at the Tamm plasmon polariton frequency for different excitation schemes have been examined. It has been demonstrated that such media can be used as narrowband absorbers based on Tamm plasmon polaritons localized at the interface between a photonic crystal and a nanocomposite with near-zero effective permittivity.
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4

Symonds, C., G. Lheureux, J. P. Hugonin, J. J. Greffet, J. Laverdant, G. Brucoli, A. Lemaitre, P. Senellart, and J. Bellessa. "Confined Tamm Plasmon Lasers." Nano Letters 13, no. 7 (June 20, 2013): 3179–84. http://dx.doi.org/10.1021/nl401210b.

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5

Vyunishev, Andrey M., Rashid G. Bikbaev, Sergey E. Svyakhovskiy, Ivan V. Timofeev, Pavel S. Pankin, Stanislav A. Evlashin, Stepan Ya Vetrov, Sergey A. Myslivets, and Vasily G. Arkhipkin. "Broadband Tamm plasmon polariton." Journal of the Optical Society of America B 36, no. 8 (July 31, 2019): 2299. http://dx.doi.org/10.1364/josab.36.002299.

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6

Plikusienė, Ieva, Ernesta Bužavaitė-Vertelienė, Vincentas Mačiulis, Audrius Valavičius, Almira Ramanavičienė, and Zigmas Balevičius. "Application of Tamm Plasmon Polaritons and Cavity Modes for Biosensing in the Combined Spectroscopic Ellipsometry and Quartz Crystal Microbalance Method." Biosensors 11, no. 12 (December 7, 2021): 501. http://dx.doi.org/10.3390/bios11120501.

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Low-cost 1D plasmonic photonic structures supporting Tamm plasmon polaritons and cavity modes were employed for optical signal enhancement, modifying the commercially available quartz crystal microbalance with dissipation (QCM-D) sensor chip in a combinatorial spectroscopic ellipsometry and quartz microbalance method. The Tamm plasmon optical state and cavity mode (CM) for the modified mQCM-D sample obtained sensitivity of ellipsometric parameters to RIU of ΨTPP = 126.78 RIU−1 and ΔTPP = 325 RIU−1, and ΨCM = 264 RIU−1 and ΔCM = 645 RIU−1, respectively. This study shows that Tamm plasmon and cavity modes exhibit about 23 and 49 times better performance of ellipsometric parameters, respectively, for refractive index sensing than standard spectroscopic ellipsometry on a QCM-D sensor chip. It should be noted that for the optical biosensing signal readout, the sensitivity of Tamm plasmon polaritons and cavity modes are comparable with and higher than the standard QCM-D sensor chip. The different origin of Tamm plasmon polaritons (TPP) and cavity mode (CM) provides further advances and can determine whether the surface (TPP) or bulk process (CM) is dominating. The dispersion relation feature of TPP, namely the direct excitation without an additional coupler, allows the possibility to enhance the optical signal on the sensing surface. To the best of our knowledge, this is the first study and application of the TPP and CM in the combinatorial SE-QCM-D method for the enhanced readout of ellipsometric parameters.
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7

Lin, Meng-Ying, Wen-Hui Xu, Rashid G. Bikbaev, Jhen-Hong Yang, Chang-Ruei Li, Ivan V. Timofeev, Wei Lee, and Kuo-Ping Chen. "Chiral-Selective Tamm Plasmon Polaritons." Materials 14, no. 11 (May 24, 2021): 2788. http://dx.doi.org/10.3390/ma14112788.

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Chiral-selective Tamm plasmon polariton (TPP) has been investigated at the interface between a cholesteric liquid crystal and a metasurface. Different from conventional TPP that occurs with distributed Bragg reflectors and metals, the chiral–achiral TPP is successfully demonstrated. The design of the metasurface as a reflective half-wave plate provides phase and polarization matching. Accordingly, a strong localized electric field and sharp resonance are observed and proven to be widely tunable.
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8

Xu, Wen-Hui, Yu-Hsun Chou, Zih-Ying Yang, Yi-Yun Liu, Min-Wen Yu, Chen-Hang Huang, Chun-Tse Chang, et al. "Tamm Plasmon‐Polariton Ultraviolet Lasers." Advanced Photonics Research 3, no. 1 (November 25, 2021): 2100120. http://dx.doi.org/10.1002/adpr.202100120.

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9

Yang, Zih-ying, Satoshi Ishii, Takahiro Yokoyama, Thang Duy Dao, Mao-guo Sun, Tadaaki Nagao, and Kuo-ping Chen. "Tamm plasmon selective thermal emitters." Optics Letters 41, no. 19 (September 21, 2016): 4453. http://dx.doi.org/10.1364/ol.41.004453.

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10

Chen, Yikai, Douguo Zhang, Liangfu Zhu, Qiang Fu, Ruxue Wang, Pei Wang, Hai Ming, Ramachandram Badugu, and Joseph R. Lakowicz. "Effect of metal film thickness on Tamm plasmon-coupled emission." Phys. Chem. Chem. Phys. 16, no. 46 (2014): 25523–30. http://dx.doi.org/10.1039/c4cp04031g.

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11

Lo, Shu-cheng, Chia-wei Lee, Ruey-lin Chern, and Pei-kuen Wei. "Hybrid modes in gold nanoslit arrays on Bragg nanostructures and their application for sensitive biosensors." Optics Express 30, no. 17 (August 4, 2022): 30494. http://dx.doi.org/10.1364/oe.465748.

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In this work, we present high-performance surface plasmonic sensors using gold nanostructures and Bragg photonic structures. The gold film on the Bragg structure provides Tamm plasmon states (TPs). The Fano coupling between higher order TPs and Bloch-wave surface plasmon polariton (BW-SPP) on the gold nanoslit array results in a new hybrid Tamm-plasmon mode. Using finite-difference time-domain calculations, we demonstrate that the hybrid mode has the advantages of high surface sensitivity of BW-SPP mode and high resonant quality of Tamm state. The calculated plasmonic field distribution shows that the hybrid mode has a similar evanescent distribution with BW-SPP mode on gold surface and TPs field in the Bragg structure. The experimental results verify that the hybrid mode has one hundred times higher wavelength sensitivity than the Tamm state. The figure of merit of the hybrid mode is five times better than the BW-SPP mode in conventional nanoslit arrays. The real-time sensorgram further confirms that the hybrid mode has a much higher sensitivity and better signal to noise ratios in the biomolecular interaction measurement.
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12

Gubaydullin, A. R., C. Symonds, J. Bellessa, K. A. Ivanov, E. D. Kolykhalova, M. E. Sasin, G. Pozina, and M. A. Kaliteevski. "Purcell effect in Tamm plasmon structures with QD emitter." Физика и техника полупроводников 52, no. 4 (2018): 467. http://dx.doi.org/10.21883/ftp.2018.04.45816.05.

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AbstractWe study Tamm plasmon structure based on GaAs/Al_0.95GaAs distributed Bragg reflector covered by thin silver layer, with active area formed by InAs quantum dots. We have measured the spectral and angular characteristics of photoluminescence and performed theoretical calculation of the spontaneous emission rate (modal Purcell factor) in the structure by using S-quantization formalism. We show that for Tamm plasmon mode the spontaneous emission can be enhanced by more than an order of magnitude, despite absorption in metallic layer.
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13

Lheureux, Guillaume, Stefano Azzini, Clementine Symonds, Pascale Senellart, Aristide Lemaître, Christophe Sauvan, Jean-Paul Hugonin, Jean-Jacques Greffet, and Joel Bellessa. "Polarization-Controlled Confined Tamm Plasmon Lasers." ACS Photonics 2, no. 7 (June 16, 2015): 842–48. http://dx.doi.org/10.1021/ph500467s.

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14

Symonds, C., A. Lemaître, E. Homeyer, J. C. Plenet, and J. Bellessa. "Emission of Tamm plasmon/exciton polaritons." Applied Physics Letters 95, no. 15 (October 12, 2009): 151114. http://dx.doi.org/10.1063/1.3251073.

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15

Lu, Hua, Yangwu Li, Zengji Yue, Dong Mao, and Jianlin Zhao. "Topological insulator based Tamm plasmon polaritons." APL Photonics 4, no. 4 (April 2019): 040801. http://dx.doi.org/10.1063/1.5088033.

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16

Lu, Hua, Yangwu Li, Han Jiao, Zhiwen Li, Dong Mao, and Jianlin Zhao. "Induced reflection in Tamm plasmon systems." Optics Express 27, no. 4 (February 13, 2019): 5383. http://dx.doi.org/10.1364/oe.27.005383.

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17

Adams, Mike, Ben Cemlyn, Ian Henning, Matthew Parker, Edmund Harbord, and Ruth Oulton. "Model for confined Tamm plasmon devices." Journal of the Optical Society of America B 36, no. 1 (December 19, 2018): 125. http://dx.doi.org/10.1364/josab.36.000125.

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18

Pykhtin, D. A., R. G. Bikbaev, I. V. Timofeev, S. Ya Vetrov, and V. F. Shabanov. "Perovskite-based solar cell in tamm plasmon-polariton structure." Доклады Российской академии наук. Физика, технические науки 514, no. 1 (August 10, 2024): 29–33. http://dx.doi.org/10.31857/s2686740024010042.

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The spectral properties of a solar cell with a photosensitive perovskite layer in a structure with a Tamm plasmon polariton localized at the boundary of a gold nanolattice and a one-dimensional photonic crystal are investigated. The influence of the parameters of the golden lattice on the surface current density and the efficiency of the proposed device is investigated. It is shown that when an aluminum substrate is replaced with a photonic crystal, a Tamm plasmon polariton is excited, which provides an increase in the surface current density by 33.7%, and efficiency by 35.1%.
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19

Lan, Huiting, Zhisheng Yu, Zesong Zheng, Shiping Feng, and Hong Su. "Study of Terahertz Sensing Performance Based on Graphene-DBR Asymmetric Structure." Journal of Physics: Conference Series 2470, no. 1 (March 1, 2023): 012023. http://dx.doi.org/10.1088/1742-6596/2470/1/012023.

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Abstract Tamm plasmon polaritons have super strong field localization, and can be directly excited by TM or TE polarized light without dispersive devices, whose related technology has become one of the research hotspots nowadays. In view of this, in this paper, a terahertz sensor device based on double-dip detection of Tamm plasmon polaritons is designed. The device is asymmetric structure, which can excite two Tamm plasmon polaritons modes with the different intrinsic energies at the interface between two DBRs and graphene. Through the optimized simulation analysis of its terahertz sensing characteristics, the results show that the reflection spectrum under this structure has two dips at 0.9THz and 1.0THz respectively, and their full widths at half maxima of 0.0361THz and 0.0131THz are relatively narrow. Moreover, their sensitivities are 0.21THz/RIU and 0.41THz/RIU, and the figure of merit can reach up to 5.69RIU−1 and 31.33RIU−1, respectively. Therefore, this research is suitable for high sensitivity terahertz double-dip detection, and has important application prospect in terahertz devices.
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20

Pyatnov, Maxim V., Rashid G. Bikbaev, Ivan V. Timofeev, Ilya I. Ryzhkov, Stepan Ya Vetrov, and Vasily F. Shabanov. "Tamm Plasmons in TiO2 Nanotube Photonic Crystals." Photonics 10, no. 1 (January 6, 2023): 64. http://dx.doi.org/10.3390/photonics10010064.

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The anodic TiO2 photonic crystals evoke great interest for application as photocatalytic media due to high absorption of light resuling from their specific structure. In this work, the optical properties of the photonic crystal based on a bamboo-type TiO2 nanotube with a metallic coating are analyzed theoretically by the finite-difference time-domain method. The occurrence of Tamm plasmons that appears as a peak in the absorption spectrum is predicted. A Tamm plasmon polariton is a localized state of light excited at the boundary of two highly reflective media, a metal and a Bragg reflector. The integral absorption of the gold-, titanium-, and titanium nitride-coated photonic crystals in the wavelength range of 450–600 nm is calculated. It is established that the titanium nitride-coated structure exhibits the maximum integral absorption.
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21

Li, Fengyu, Jiao Xu, Wei Li, Jianbo Li, Yuxiang Peng, and Mengdong He. "Tunable Low-Threshold Optical Bistability in Optical Tamm Plasmon Superlattices." Coatings 13, no. 5 (May 17, 2023): 938. http://dx.doi.org/10.3390/coatings13050938.

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We propose a scheme to obtain tunable low-threshold optical bistability of reflected beams in optical Tamm plasmon superlattices (TPS). The low-threshold optical bistability is triggered due to the strong third-order non-linearity of graphene and the local field enhancement in the TPS. Our results show that the optical Tamm plasmon superlattices have the ability to lower the bistable threshold even further than the single optical Tamm state. The results show that the hysteresis behavior and optical bistability threshold can be continuously adjusted by changing the applied voltage and the number of graphene layers (N ≤ 4). In particular, the optical bistability in the TPS is affected by the incident angle. Our results introduce a new possible route for low threshold optical bistability in the THz range and provide a new method in the field of all-optical switching applications.
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22

Tsung, Cheng-Sheng, Jiann-Yeu Chen, Shao-Wen Hung, Ching-Yu Tu, Hsin-Yu Chou, Wei-Hsiang Chiang, and Dong-Sing Wuu. "Individual characteristics and gain ratios of surface plasmon resonance and Tamm plasmon resonance in optical Tamm states." Materials Science in Semiconductor Processing 188 (March 2025): 109243. https://doi.org/10.1016/j.mssp.2024.109243.

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23

Bikbaev, Rashid G., Dmitrii N. Maksimov, Kuo-Ping Chen, and Ivan V. Timofeev. "Double-Resolved Beam Steering by Metagrating-Based Tamm Plasmon Polariton." Materials 15, no. 17 (August 31, 2022): 6014. http://dx.doi.org/10.3390/ma15176014.

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We consider Tamm plasmon polariton in a subwavelength grating patterned on top of a Bragg reflector. We demonstrate dynamic control of the phase and amplitude of a plane wave reflected from such metagrating due to resonant coupling with the Tamm plasmon polariton. The tunability of the phase and amplitude of the reflected wave arises from modulation of the refractive index of a transparent conductive oxide layer by applying the bias voltage. The electrical switching of diffracted beams of the ±1st order is shown. The possibility of doubling the angular resolution of beam steering by using asymmetric reflected phase distribution with integer and half-integer periods of the metagrating is demonstrated.
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24

Jeng, Shie-Chang. "Applications of Tamm plasmon-liquid crystal devices." Liquid Crystals 47, no. 8 (March 2, 2020): 1223–31. http://dx.doi.org/10.1080/02678292.2020.1733114.

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25

Sasin, M. E., R. P. Seisyan, M. A. Kaliteevski, S. Brand, R. A. Abram, J. M. Chamberlain, I. V. Iorsh, et al. "RETRACTED: Tamm plasmon-polaritons: First experimental observation." Superlattices and Microstructures 47, no. 1 (January 2010): 44–49. http://dx.doi.org/10.1016/j.spmi.2009.09.003.

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26

Huang, Syuan-Guei, Kuo-Ping Chen, and Shie-Chang Jeng. "Phase sensitive sensor on Tamm plasmon devices." Optical Materials Express 7, no. 4 (March 15, 2017): 1267. http://dx.doi.org/10.1364/ome.7.001267.

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27

Azzini, Stefano, Guillaume Lheureux, Clementine Symonds, Jean-Michel Benoit, Pascale Senellart, Aristide Lemaitre, Jean-Jacques Greffet, Cedric Blanchard, Christophe Sauvan, and Joel Bellessa. "Generation and Spatial Control of Hybrid Tamm Plasmon/Surface Plasmon Modes." ACS Photonics 3, no. 10 (September 21, 2016): 1776–81. http://dx.doi.org/10.1021/acsphotonics.6b00521.

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28

Wang, Jiaying, Yisong Zhu, Wenhao Wang, Yunze Li, Rui Gao, Peng Yu, Hongxing Xu, and Zhiming Wang. "Broadband Tamm plasmon-enhanced planar hot-electron photodetector." Nanoscale 12, no. 47 (2020): 23945–52. http://dx.doi.org/10.1039/d0nr06294d.

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29

Bikbaev, Rashid, Stepan Vetrov, and Ivan Timofeev. "Two Types of Localized States in a Photonic Crystal Bounded by an Epsilon near Zero Nanocomposite." Photonics 5, no. 3 (August 9, 2018): 22. http://dx.doi.org/10.3390/photonics5030022.

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The spectral properties of a one-dimensional photonic crystal bounded by a resonant absorbing nanocomposite layer with the near-zero permittivity have been studied. The problem of calculating the transmittance, reflectance, and absorptance spectra of such structures at the normal and oblique incidence of light has been solved. It is shown that, depending on the permittivity sign near zero, the nanocomposite is characterized by either metallic or dielectric properties. The possibility of simultaneous formation of the Tamm plasmon polariton at the photonic crystal/metallic nanocomposite interface and the localized state similar to the defect mode with the field intensity maximum inside the dielectric nanocomposite layer is demonstrated. Specific features of field localization at the Tamm plasmon polariton and defect mode frequencies are analyzed.
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30

Almawgani, Abdulkarem H. M., Hussein A. Elsayed, Ahmed Mehaney, T. A. Taha, Ziyad Awadh Alrowaili, Ghassan Ahmed Ali, Walied Sabra, Sayed Asaduzzaman, and Ashour M. Ahmed. "Photonic crystal nanostructure as a photodetector for NaCl solution monitoring: theoretical approach." RSC Advances 13, no. 10 (2023): 6737–46. http://dx.doi.org/10.1039/d3ra00308f.

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In this research, we have a theoretical simple and highly sensitive sodium chloride (NaCl) sensor based on the excitation of Tamm plasmon resonance through a one-dimensional photonic crystal structure.
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31

Morrone, Josefina, Juan Ignacio Ramallo, Diego F. Lionello, Andrés Zelcer, Baptiste Auguié, Paula C. Angelomé, and M. Cecilia Fuertes. "Incorporation of porous protective layers as a strategy to improve mechanical stability of Tamm plasmon based detectors." Materials Advances 2, no. 8 (2021): 2719–29. http://dx.doi.org/10.1039/d1ma00079a.

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A strategy to protect Tamm plasmon optical detectors from mechanical stress and handling by adding a sol–gel porous oxide overlayer is demonstrated. The sensing properties of the protected devices are also shown.
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32

Chen, Yikai, Douguo Zhang, Liangfu Zhu, Ruxue Wang, Pei Wang, Hai Ming, Ramachandram Badugu, and Joseph R. Lakowicz. "Tamm plasmon- and surface plasmon-coupled emission from hybrid plasmonic–photonic structures." Optica 1, no. 6 (December 11, 2014): 407. http://dx.doi.org/10.1364/optica.1.000407.

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33

Gessler, J., V. Baumann, M. Emmerling, M. Amthor, K. Winkler, S. Höfling, C. Schneider, and M. Kamp. "Electro optical tuning of Tamm-plasmon exciton-polaritons." Applied Physics Letters 105, no. 18 (November 3, 2014): 181107. http://dx.doi.org/10.1063/1.4901023.

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34

Zhang, Wei Li, Fen Wang, Yun Jiang Rao, and Yao Jiang. "Novel sensing concept based on optical Tamm plasmon." Optics Express 22, no. 12 (June 5, 2014): 14524. http://dx.doi.org/10.1364/oe.22.014524.

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35

Homeyer, Estelle, Clémentine Symonds, Aristide Lemaître, Jean-Claude Plenet, and Joel Bellessa. "Strong coupling between Tamm plasmon and QW exciton." Superlattices and Microstructures 49, no. 3 (March 2011): 224–28. http://dx.doi.org/10.1016/j.spmi.2010.06.007.

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36

Sasin, M. E., R. P. Seisyan, M. A. Kalitteevski, S. Brand, R. A. Abram, J. M. Chamberlain, A. Yu Egorov, A. P. Vasil’ev, V. S. Mikhrin, and A. V. Kavokin. "Tamm plasmon polaritons: Slow and spatially compact light." Applied Physics Letters 92, no. 25 (June 23, 2008): 251112. http://dx.doi.org/10.1063/1.2952486.

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37

Bikbaev, Rashid G., Stepan Ya Vetrov, and Ivan V. Timofeev. "Hyperbolic metamaterial for the Tamm plasmon polariton application." Journal of the Optical Society of America B 37, no. 8 (July 7, 2020): 2215. http://dx.doi.org/10.1364/josab.394935.

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38

Gazzano, O., S. Michaelis de Vasconcellos, K. Gauthron, C. Symonds, P. Voisin, J. Bellessa, A. Lemaître, and P. Senellart. "Single photon source using confined Tamm plasmon modes." Applied Physics Letters 100, no. 23 (June 4, 2012): 232111. http://dx.doi.org/10.1063/1.4726117.

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39

Morozov, K. M., K. A. Ivanov, N. Selenin, S. Mikhrin, D. de Sa Pereira, C. Menelaou, A. P. Monkman, and M. A. Kaliteevski. "Purcell effect investigation in organic Tamm plasmon structures." Journal of Physics: Conference Series 1135 (December 2018): 012082. http://dx.doi.org/10.1088/1742-6596/1135/1/012082.

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40

Rudakova, Natalya V., Rashid G. Bikbaev, Larisa E. Tyryshkina, Stepan Ya Vetrov, and Ivan V. Timofeev. "Tuning Q-Factor and Perfect Absorption Using Coupled Tamm States on Polarization-Preserving Metasurface." Photonics 10, no. 12 (December 18, 2023): 1391. http://dx.doi.org/10.3390/photonics10121391.

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The circular polarization of light flips its handedness after a conventional metallic mirror reflection. Therefore, a polarization-preserving metasurface is a crucially important element in a series of chiral photonic structures. They include tunable cholesteric LCs and anisotropic photonic crystals. Chiral structures are rich in interfacial localized modes including Tamm states. In this report, coupled modes formed as a result of the interaction between two chiral optical Tamm states or a chiral optical Tamm state and a chiral Tamm plasmon polariton are analytically and numerically investigated. It is shown that the effective control of coupled modes can be carried out by changing the pitch of the cholesteric and the angle between the optical axis of the cholesteric and the polarization-preserving anisotropic mirror. The influence of the metasurface period on the spectral characteristics of coupled modes is investigated. The possibility of realizing a bound state in the continuum of the Friedrich–Wintgen type, resulting from the destructive interference of coupled modes, which leads to the collapse of the resonance line corresponding to the chiral optical Tamm state, has been demonstrated.
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41

Liu, Xiangjun, Jingxu Shi, Yixuan Wang, Shiyao Sun, and Xiangfu Wang. "Highly Tunable Light Absorber Based on Topological Interface Mode Excitation of Optical Tamm State." Sensors 24, no. 17 (September 5, 2024): 5772. http://dx.doi.org/10.3390/s24175772.

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Optical absorbers based on Tamm plasmon states are known for their simple structure and high operational efficiency. However, these absorbers often have limited absorption channels, and it is challenging to continuously adjust their light absorption rates. Here, we propose a Tamm plasmon state optical absorber composed of a layered stack structure consisting of one-dimensional topological photonic crystals and graphene nano-composite materials. Using the four-by-four transfer matrix method, we investigate the structural relationship of the absorber. Our results reveal that topological interface states (TISs) effectively excite the optical Tamm state (OTS), leading to multiple absorption peaks. This expands the number of absorption channels, with the coupling number of the TIS determining the transmission quality of these channels—a value further adjustable by the period number of the photonic crystals. Tuning the filling factor, refractive index, and thickness of the graphene nano-composite material allows for a wide range of control over the device’s absorption rate, from 0 to 1. Additionally, adjusting the defect layer thickness, incident angle, and Fermi energy enables us to control the absorber’s operational bandwidth and the switching of its absorption effect. This work presents a new approach to expanding the tunability of optoelectronic devices.
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42

Srivastava, Triranjita, Swapnil Chitriv, Subrat Sahu, Pintu Gorai, and Rajan Jha. "Photonic spin Hall effect using hybrid Tamm plasmon polariton." Journal of Applied Physics 132, no. 20 (November 28, 2022): 203103. http://dx.doi.org/10.1063/5.0123612.

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Here, we report a photonic spin Hall effect (PSHE), i.e., splitting of opposite spin in a transverse direction using a multi-layered metallo-dielectric heterostructure by hybridization of a Tamm plasmon polariton and a surface plasmon polariton. The underlying mechanism of PSHE is also explained using the concept of superposition of normal and abnormal modes in the circular-polarization basis. It is revealed that the spin-dependent transverse shift for the proposed hybrid structure is enormously high owing to the transverse shift of ∼18 μm . The PSHE is found to be strongly dependent on the number of bi-layers of the structure and the analyte refractive index, which provides an additional degree of freedom for tailoring the device performance. Therefore, this study opens a pathway for developing next-generation photonic spin Hall devices in the fields of spin photonics, optical sensing, and optical communications.
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43

Pühringer, Gerald, and Bernhard Jakoby. "Highly Selective CMOS-Compatible Mid-Infrared Thermal Emitter/Detector Slab Design Using Optical Tamm-States." Materials 12, no. 6 (March 20, 2019): 929. http://dx.doi.org/10.3390/ma12060929.

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In this work, we propose and evaluate a concept for a selective thermal emitter based on Tamm plasmons suitable for monolithic on-chip integration and fabrication by conventional complementary metal oxide semiconductor (CMOS)-compatible processes. The original design of Tamm plasmon structures features a purely one-dimensional array of layers including a Bragg mirror and a metal. The resonant field enhancement next to the metal interface corresponding to optical Tamm states leads to resonant emission at the target wavelength, which depends on the lateral dimensions of the bandgap structure. We demonstrate the application of this concept to a silicon slab structure instead of deploying extended one dimensional layers thus enabling coupling into slab waveguides. Here we focus on the mid-infrared region for absorption sensing applications, particularly on the CO2 absorption line at 4.26 µm as an example. The proposed genetic-algorithm optimization process utilizing the finite-element method and the transfer-matrix method reveals resonant absorption in case of incident modes guided by the slab and, by Kirchhoff’s law, corresponds to emittance up to 90% depending on different choices of the silicon slab height when the structure is used as a thermal emitter. Although we focus on the application as an emitter in the present work, the structure can also be operated as an absorber providing adjusted lateral dimensions and/or exchanged materials (e.g., a different choice for metal).
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44

Das, Ritwick, Triranjita Srivastava, and Rajan Jha. "Tamm-plasmon and surface-plasmon hybrid-mode based refractometry in photonic bandgap structures." Optics Letters 39, no. 4 (February 10, 2014): 896. http://dx.doi.org/10.1364/ol.39.000896.

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45

Almeida, Miguel A. S., João P. M. Carvalho, Isabel Pastoriza-Santos, José M. M. M. Almeida, and Luís C. C. Coelho. "A Comparative Study of Surface Plasmon and Tamm Plasmon Polaritons for Hydrogen Sensing." EPJ Web of Conferences 305 (2024): 00020. http://dx.doi.org/10.1051/epjconf/202430500020.

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Due to the exponential increase in energy consumption and CO2 emissions, new sustainable energy sources have emerged, and hydrogen (H2) is one of them. Despite all the advantages, H2 has high flammability, so constant monitoring is essential. Two optical techniques were numerically studied and compared with the goal of H2 sensing: surface plasmon polaritons (SPP) and Tamm plasmon polaritons (TPP). The H2-sensitive material used was palladium (Pd) in both techniques. The SPP structure was found to have more sensitivity to H2 than TPP, 23 and 5nm/4vol% H2, respectively. However, the latter has lower FWHM, with the minimum of the band showing reflectivity near 0%. In addition, TPP also uses more costeffective materials and can be interrogated at normal incidence with depolarized light. The potential of using each of these optical techniques for H2 sensing was demonstrated.
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46

Bikbaev, Rashid G., Kuo-Ping Chen, and Ivan V. Timofeev. "Two-Dimensional Dynamic Beam Steering by Tamm Plasmon Polariton." Photonics 10, no. 10 (October 13, 2023): 1151. http://dx.doi.org/10.3390/photonics10101151.

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The dynamic steering of a beam reflected from a photonic structure supporting Tamm plasmon polariton is demonstrated. The phase and amplitude of the reflected wave are adjusted by modulating the refractive index of a transparent conductive oxide layer by applying a bias voltage. It is shown that the proposed design allows for two-dimensional beam steering by deflecting the light beam along the polar and azimuthal angles.
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47

Pugh, J. R., E. G. H. Harbord, A. Sarua, P. S. Fletcher, Y. Tian, T. Wang, and M. J. Cryan. "A Tamm plasmon-porous GaN distributed Bragg reflector cavity." Journal of Optics 23, no. 3 (February 18, 2021): 035003. http://dx.doi.org/10.1088/2040-8986/abdccb.

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48

Juneau-Fecteau, Alexandre, Rémy Savin, Abderraouf Boucherif, and Luc G. Fréchette. "A practical Tamm plasmon sensor based on porous Si." AIP Advances 11, no. 6 (June 1, 2021): 065305. http://dx.doi.org/10.1063/5.0054629.

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49

Lin, Zhenhui, Haizhou Liu, Tong Qiao, Guozhi Hou, Hui Liu, Jun Xu, Jia Zhu, and Lin Zhou. "Tamm plasmon enabled narrowband thermal emitter for solar thermophotovoltaics." Solar Energy Materials and Solar Cells 238 (May 2022): 111589. http://dx.doi.org/10.1016/j.solmat.2022.111589.

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50

Maji, Partha Sona, and Ritwick Das. "Hybrid-Tamm-Plasmon-Polariton Based Self-Reference Temperature Sensor." Journal of Lightwave Technology 35, no. 14 (July 15, 2017): 2833–39. http://dx.doi.org/10.1109/jlt.2017.2705910.

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