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Journal articles on the topic 'Metal-dielectric structures'

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1

Lapchinskiy, V. I., A. V. Machulyanskiy, D. D. Tatarchuk, and T. L. Volkhova. "Metal-dielectric nanocomposite structures." Electronics and Communications 16, no. 1 (2011): 20–22. http://dx.doi.org/10.20535/2312-1807.2011.16.1.273858.

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The influence of nanocomposite structures Al-polymer at its dielectric properties in microwave range is investigated. The graphs of experimental dependences of transmission and reflection coefficients of electromagnetic waves, the real and the imaginary part of dielectric permittivity of the samples, as well as of the volume fraction of the dispersed phase are represented
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2

Gomeniuk, Y. V. "Current transport mechanisms in metal – high-k dielectric – silicon structures." Semiconductor Physics Quantum Electronics and Optoelectronics 15, no. 2 (2012): 139–46. http://dx.doi.org/10.15407/spqeo15.02.139.

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3

Sasin, M. E., N. D. Il’inskaya, Yu M. Zadiranov, et al. "Cylindrical multilayer metal–dielectric structures." Technical Physics Letters 41, no. 11 (2015): 1097–98. http://dx.doi.org/10.1134/s1063785015110255.

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4

M.V. Davidovich. "Resonant tunneling of photons in layered optical nanostructures (metamaterials)." Technical Physics 68, no. 4 (2023): 462. http://dx.doi.org/10.21883/tp.2023.04.55937.275-22.

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The conditions of resonant (almost complete) tunneling of photons (plane monochromatic electromagnetic waves) through layered dielectric and metal-dielectric structures are considered. Resonant tunneling occurs at frequencies at which the resonance conditions for the corresponding structures of open resonators are met. For metal-dielectric structures, the possibility of tunneling in the optical range with a strong barrier in the IR range is shown, which can be used to control the transmission of window panes. Keywords: dielectric permittivity, homogenization, resonant tunneling, plasmons, meta
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5

Kostrobij, P., and V. Polovyi. "Surface plasmon polaritons in dielectric/metal/dielectric structures: metal layer thickness influence." Mathematical Modeling and Computing 6, no. 1 (2019): 109–15. http://dx.doi.org/10.23939/mmc2019.01.109.

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6

Frisbie, S. P., A. Krishnan, Xiaoyan Xu, et al. "Optical Reflectivity of Asymmetric Dielectric–Metal–Dielectric Planar Structures." Journal of Lightwave Technology 27, no. 15 (2009): 2964–69. http://dx.doi.org/10.1109/jlt.2008.2009886.

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7

Ovchinnikov, Victor, and Andriy Shevchenko. "Self-Organization-Based Fabrication of Stable Noble-Metal Nanostructures on Large-Area Dielectric Substrates." Journal of Chemistry 2013 (2013): 1–10. http://dx.doi.org/10.1155/2013/158431.

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A cost-effective fabrication of random noble-metal nanostructures with a feature size of the order of 10 nm on a large-area dielectric substrate is described. The method combines dry etching of the substrate through a self-organized metal mask with a directional deposition of a multilayered metal film. The technique allows one to create metal nanoislands on a nanopatterned dielectric template with an enhanced adhesion between the metal and the dielectric. The use of the adhesion layer—that makes the structures stable—is important in view of variety of optical and other potential applications o
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8

Hino, Taro. "Power Source of Metal-Ultrathin Dielectric Film-Metal Structures." Japanese Journal of Applied Physics 35, Part 1, No. 10 (1996): 5400–5404. http://dx.doi.org/10.1143/jjap.35.5400.

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9

Давидович, М. В. "Резонансное туннелирование фотонов в слоистых оптических наноструктурах (метаматериалах)". Журнал технической физики 93, № 4 (2023): 495. http://dx.doi.org/10.21883/jtf.2023.04.55037.275-22.

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The conditions of resonant (almost complete) tunneling of photons (plane monochromatic electromagnetic waves) through layered dielectric and metal-dielectric structures are considered. Resonant tunneling occurs at frequencies at which the resonance conditions for the corresponding structures of open resonators are met. For metal-dielectric structures, the possibility of tunneling in the optical range with a strong barrier in the IR range is shown, which can be used to control the transmission of window panes.
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10

Kashapov, A. I., E. A. Bezus, D. A. Bykov, and L. L. Doskolovich. "Differentiation of optical signals using an integrated metal-dielectric-metal structure." Izvestiâ Akademii nauk SSSR. Seriâ fizičeskaâ 88, no. 1 (2024): 5–10. http://dx.doi.org/10.31857/s0367676524010015.

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We consider optical properties of integrated metal-dielectric-metal structures embedded in a dielectric slab waveguide and their application to the problems of first- and second-order optical differentiation of the profile of the incident optical beam in reflection. According to the presented numerical simulation results, the investigated structures enable performing the spatial differentiation operation with high quality. The presented results may find application in novel systems for optical information processing and analog optical computing based on integrated nanophotonic structures.
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11

YUROVA, V. A., M. N. BUKINA, Yu V. CHURKIN, A. B. FEDORTSOV, and G. L. KLIMCHITSKAYA. "CASIMIR PRESSURE IN MDS-STRUCTURES." International Journal of Modern Physics: Conference Series 14 (January 2012): 566–75. http://dx.doi.org/10.1142/s2010194512007702.

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The Casimir pressure on the dielectric layer in metal-dielectric-semiconductor (MDS) structures is calculated in the framework of the Lifshitz theory at nonzero temperature. In this calculation the standard parameters of semiconductor devices with a thin dielectric layer are used. We consider the thickness of a layer decreasing from 40 to 1 nm. At the shortest thickness the Casimir pressure achieves 8 MPa. At small thicknesses the results are compared with the predictions of nonrelativistic theory.
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12

Afanasiev M. S., Belorusov D.A., Kiselev D. A., Sivov A. A., and Chucheva G. V. "The influence of the PZT buffer layer on electrophysical properties OF MDM structures with the BST film." Physics of the Solid State 63, no. 13 (2022): 1757. http://dx.doi.org/10.21883/pss.2022.13.52318.161.

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Films of the composition Ba0.8Sr0.2TiO3 (BST) were synthesized by the method of high-frequency (HF) sputtering on the buffer layer of a ferroelectric film of the composition PbZrxTi1-xO3 (PZT). Comparative results of electrophysical properties of three different metal--dielectric--metal (MDM)-structures are presented: Pt/BST/Ni, Pt/PZT/Ni, and Pt/PZT-BST/Ni. Keywords: metal--dielectric--metal structures, ferroelectric films of composition Ba0.8Sr0.2TiO3, a buffer layer, electrophysical properties.
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13

Afanasiev M. S., Belorusov D.A., Kiselev D. A., Sivov A. A., and Chucheva G. V. "The influence of the PZT buffer layer on electrophysical properties of MDM structures with the BST film." Physics of the Solid State 63, no. 13 (2022): 2190. http://dx.doi.org/10.21883/pss.2022.13.54696.161.

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Films of the composition Ba0.8Sr0.2TiO3 (BST) were synthesized by the method of high-frequency (HF) sputtering on the buffer layer of a ferroelectric film of the composition PbZrxTi1-xO3 (PZT). Comparative results of electrophysical properties of three different metal--dielectric--metal (MDM)-structures are presented: Pt/BST/Ni, Pt/PZT/Ni, and Pt/PZT-BST/Ni. Keywords: metal--dielectric--metal structures, ferroelectric films of composition Ba0.8Sr0.2TiO3, a buffer layer, electrophysical properties.
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14

Szentirmay, Z. "Surface plasmon spectroscopy of metal/dielectric structures." Spectrochimica Acta Part A: Molecular Spectroscopy 48, no. 1 (1992): 9–17. http://dx.doi.org/10.1016/0584-8539(92)80192-y.

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15

Bezuglyj, A. I., I. V. Mironenko, and V. A. Shklovskij. "Effective cross-plane thermal conductivity of metal-dielectric multilayers at low temperatures." Low Temperature Physics 50, no. 4 (2024): 320–27. http://dx.doi.org/10.1063/10.0025298.

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Heat transfer in layered metal-dielectric structures is considered theoretically based on an analytical solution of the Boltzmann transfer equation for the phonon distribution function. Taking into account the size effect, the problem of effective cross-plane thermal conductivity of structures containing two metal layers is analyzed in detail. If the thickness of the metal layers is less than the phonon mean free path, interlayer heat transfer is carried out predominantly by phonons, and the effective cross-plane thermal conductivity is determined by the reflection of phonons from the metal/di
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16

Kharlamov, V. F., D. A. Korostelev, I. G. Bogoraz, O. I. Markov, and Yu V. Khripunov. "Electric conductivity of metal-dielectric-metal structures with dielectric layer formed by spherical metal oxide nanoparticles." Technical Physics Letters 37, no. 6 (2011): 511–14. http://dx.doi.org/10.1134/s106378501106006x.

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17

Lopéz, I. Pérez, L. Cattin, D. T. Nguyen, M. Morsli, and J. C. Bernède. "Dielectric/metal/dielectric structures using copper as metal and MoO3 as dielectric for use as transparent electrode." Thin Solid Films 520, no. 20 (2012): 6419–23. http://dx.doi.org/10.1016/j.tsf.2012.06.056.

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18

Nesterenko, D. V., A. A. Morozov, and L. L. Doskolovich. "Optical image edge detection by transmissive metal-dielectric-metal structures." Computer Optics 5, no. 45 (2021): 678–84. http://dx.doi.org/10.18287/2412-6179-co-853.

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The feasibility of an optical image edge detection based on metal-insulator-metal (MIM) resonance transmission structures is experimentally investigated. The structures are fabricated on a glass substrate and consist of thin aluminum layers separated by a quartz layer. The excitation of Fabry-Perot modes by an incident wave produces resonance line shapes in angular and wavelength transmission spectra. Resonance enhancement and suppression of beams using the MIM structures can be implemented for suppressing the illuminating beam and amplifying the field scattered by an object. By using the MIM
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19

Nesterenko, D. V., A. A. Morozov, and L. L. Doskolovich. "Optical image edge detection by transmissive metal-dielectric-metal structures." Computer Optics 5, no. 45 (2021): 678–84. http://dx.doi.org/10.18287/2412-6179-co-853.

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The feasibility of an optical image edge detection based on metal-insulator-metal (MIM) resonance transmission structures is experimentally investigated. The structures are fabricated on a glass substrate and consist of thin aluminum layers separated by a quartz layer. The excitation of Fabry-Perot modes by an incident wave produces resonance line shapes in angular and wavelength transmission spectra. Resonance enhancement and suppression of beams using the MIM structures can be implemented for suppressing the illuminating beam and amplifying the field scattered by an object. By using the MIM
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20

Tatmyshevskiy, Mikhail K., Dmitry I. Yakubovsky, Olesya O. Kapitanova, et al. "Hybrid Metal-Dielectric-Metal Sandwiches for SERS Applications." Nanomaterials 11, no. 12 (2021): 3205. http://dx.doi.org/10.3390/nano11123205.

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The development of efficient plasmonic nanostructures with controlled and reproducible surface-enhanced Raman spectroscopy (SERS) signals is an important task for the evolution of ultrasensitive sensor-related methods. One of the methods to improving the characteristics of nanostructures is the development of hybrid structures that include several types of materials. Here, we experimentally investigate ultrathin gold films (3–9 nm) near the percolation threshold on Si/Au/SiO2 and Si/Au/SiO2/graphene multilayer structures. The occurring field enhanced (FE) effects were characterized by a record
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21

Sarychev, Andrey, Andrey Ivanov, Andrey Lagarkov, and Grégory Barbillon. "Light Concentration by Metal-Dielectric Micro-Resonators for SERS Sensing." Materials 12, no. 1 (2018): 103. http://dx.doi.org/10.3390/ma12010103.

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Metal-dielectric micro/nano-composites have surface plasmon resonances in visible and near-infrared domains. Excitation of coupled metal-dielectric resonances is also important. These different resonances can allow enhancement of the electromagnetic field at a subwavelength scale. Hybrid plasmonic structures act as optical antennae by concentrating large electromagnetic energy in micro- and nano-scales. Plasmonic structures are proposed for various applications such as optical filters, investigation of quantum electrodynamics effects, solar energy concentration, magnetic recording, nanolasing,
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22

Wen-jing, CAO, SUN Li-ze-tong, GUO Fu-zhou, et al. "Enhancing the fluorescence emission by flexible metal-dielectric-metal structures." Chinese Optics 15, no. 1 (2022): 1–17. http://dx.doi.org/10.37188/co.en.2021-0084.

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23

Yarmarkin, V. K., and S. P. Teslenko. "Dielectric relaxation in thin-film metal-PZT-ferroelectric-metal structures." Physics of the Solid State 40, no. 10 (1998): 1738–41. http://dx.doi.org/10.1134/1.1130647.

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24

Kostrobij, P., V. Pavlysh, D. Nevinskyi, and V. Polovyi. "SPP waves in "dielectric-metal-dielectric" structures: influence of exchange correlations." Mathematical Modeling and Computing 4, no. 2 (2017): 148–55. http://dx.doi.org/10.23939/mmc2017.02.148.

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25

Jiang, Xiangqian, Haiming Yuan, Bing Zhang, and Xiudong Sun. "Coupling properties between plasmonic modes and cavity modes in corrugated metal–dielectric–metal waveguide." RSC Advances 6, no. 106 (2016): 104112–16. http://dx.doi.org/10.1039/c6ra21926h.

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26

Dutta Choudhury, Sharmistha, Ramachandram Badugu, Krishanu Ray, and Joseph R. Lakowicz. "Directional Emission from Metal–Dielectric–Metal Structures: Effect of Mixed Metal Layers, Dye Location, and Dielectric Thickness." Journal of Physical Chemistry C 119, no. 6 (2015): 3302–11. http://dx.doi.org/10.1021/jp512174w.

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27

Polovyi, Vitalii, and Kostrobiy Petro. "The influence of the electroneutrality of the metal layer on the plasmon spectrum in "dielectric-metal-dielectric" structures." Modeling, Control and Information Technologies, no. 3 (November 5, 2019): 141–44. http://dx.doi.org/10.31713/mcit.2019.19.

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This paper proposes a model that takes into account the discretization of the Fermi wave vector and energy levels, as well as the condition of electroneutrality when investigating the influence of metal thickness on the spectrum of SPPs waves in heterogeneous dielectric-metal-dielectric structures.
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28

Sitanov, Dmitry, and Daniil Blinov. "Metal content monitoring in the biological structures." From Chemistry Towards Technology Step-By-Step 5, no. 1 (2024): 137–44. http://dx.doi.org/10.52957/2782-1900-2024-5-1-137-144.

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The authors propose a monitoring method for defining metal content in the biological structures, such as plant leaves, tissue samples of animal origin, human skin, etc. The authors used dielectric barrier discharge (DBD) in air at atmospheric pressure as a diagnostic medium. According to the research, at the optimal selection of gas discharge parameters it will not have destructive effect on tissues of biological structure. Indeed, generation of chemically active particles in the plasma will be minimal one. The dielectric barrier separates the investigated sample from the electrode of the disc
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29

Morozov, V. M., V. I. Magro, and E. Yu Trakhtman. "Infinite linear waveguide antenna array with metal-dielectric structures in the "floquet channel"." Journal of Physics and Electronics 28, no. 1 (2020): 91–96. http://dx.doi.org/10.15421/332015.

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An electrodynamics calculation is performed for an infinite waveguide antenna array in the form of open ends of waveguides, in the near zone of which a metal-dielectric structure is located. This metal-dielectric structure is located in the "Floquet channels" and is a combination of a dielectric coating over the antenna array and horns. In this case, the horns are not a continuation of the waveguides, but are located at some distance from them. The space between the waveguides and the horns is filled with a dielectric. A system of equations that allows calculating the reflection coefficients o
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30

Fonseca, L. R. C., PY Prodhomme, and P. Blaise. "Bridging Electrical and Structural Interface Properties: a Combined DFT-GW Approach." Journal of Integrated Circuits and Systems 2, no. 2 (2007): 94–103. http://dx.doi.org/10.29292/jics.v2i2.273.

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The selection of a proper metal for replacement of polycrystalline silicon as the metal gate in future generation transistors has been hampered by pinning of the metal Fermi level at the metal/dielectric interface. Using monoclinic hafnia and zirconia as the gate dielectric we compare three different metal gate/gate dielectric interface structures where the oxygen affinity of the metal gate varies from low to high under normal processing conditions. For each of the metal gate/gate dielectric combination we considered a number of interface stoichiometries and tried to identify the most likely i
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31

Teguh Puja Negara, Hendradi Hardhienata, Akhiruddin Maddu, and Husin Alatas. "Design Simulation of Multilayer Structures for the Development of Biosensor Based on Transverse Matrix Method." International Journal of Nanoelectronics and Materials (IJNeaM) 16, DECEMBER (2023): 43–49. http://dx.doi.org/10.58915/ijneam.v16idecember.384.

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Simulation of electromagnetic wave propagation on layered metal-dielectric structures using analytical methods is a study that continues to be developed because it involves strict mathematical equations with exact results. In this study, the transfer matrix method was developed to analyze the dielectric-metal-metal-dielectric structure through the reflection profile. The emergence of the Surface Plasmons Resonance (SPR) phenomenon causes a minimum reflectance whose changes are analyzed through variations in optical and physical parameters. The simulation shows that the minimum reflectance angl
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32

Davoyan, Artur R., Ilya V. Shadrivov, Andrey A. Sukhorukov, and Yuri S. Kivshar. "Plasmonic Bloch oscillations in chirped metal-dielectric structures." Applied Physics Letters 94, no. 16 (2009): 161105. http://dx.doi.org/10.1063/1.3119666.

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33

Choi, Geun-Su, Eun-Jeong Bae, Byeong-Kwon Ju, and Young-Wook Park. "Enhancing Light Extraction Efficiency in OLED Using Scattering Structure-Embedded DMD-Based Transparent Composite Electrodes." Nanomaterials 13, no. 15 (2023): 2253. http://dx.doi.org/10.3390/nano13152253.

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This study investigates the application of scattering structures to the metal layer in a DMD (Dielectric/Metal/Dielectric) configuration through plasma treatment. The purpose is to enhance the light extraction efficiency of organic light-emitting diodes (OLEDs). Different plasma conditions were explored to create scattering structures on the metal layer. The fabricated devices were characterized for their electrical and optical properties. The results demonstrate that the introduction of scattering structures through plasma treatment effectively improves the light extraction efficiency of OLED
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34

Gökçen, Muharrem, and Mert Yıldırım. "The effects of Bi4Ti3O12 interfacial ferroelectric layer on the dielectric properties of Au/n-Si structures." International Journal of Modern Physics B 29, no. 18 (2015): 1550120. http://dx.doi.org/10.1142/s0217979215501209.

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Au/n-Si metal-semiconductor (MS) and Au/Bi4Ti3O12/n-Si metal-ferroelectric-semiconductor (MFS) structures were fabricated and admittance measurements were held between 5 kHz and 1 MHz at room temperature so that dielectric properties of these structures could be investigated. The ferroelectric interfacial layer Bi4Ti3O12 decreased the polarization voltage by providing permanent dipoles at metal/semiconductor interface. Depending on different mechanisms, dispersion behavior was observed in dielectric constant, dielectric loss and loss tangent versus bias voltage plots of both MS and MFS structu
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35

Afanasyev M. S., Belorusov D. A., Kiselev D. A., and Chucheva G. V. "Influence of the upper electrode material on the electrophysical properties of MDM structures based on ferroelectric films." Physics of the Solid State 65, no. 6 (2023): 1015. http://dx.doi.org/10.21883/pss.2023.06.56117.73.

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Ferroelectric films of the composition Ba0.8Sr0.2TiO3 (BST) were synthesized on platinized silicon substrates by RF sputtering. Top electrodes made of nickel, aluminum, copper and chromium were formed on the grown films by electron beam sputtering. The results of studies of the electrophysical properties of the obtained metal-dielectric-metal (MDM) heterostructures (Me-BST-Pt-Si) are presented. Keywords: ferroelectric BST films, metal-dielectric-metal (MDM) structures, microstructure, electrophysical properties.
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36

Vu, K. T. C., G. M. Kazaryan, and V. L. Savvin. "Modeling Metal–Dielectric–Metal Structures for the Detection of Terahertz Radiation." Bulletin of the Russian Academy of Sciences: Physics 85, no. 1 (2021): 65–69. http://dx.doi.org/10.3103/s1062873821010275.

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37

Chen, N. C., C. Y. Lu, Y. L. Huang, C. C. Liao, W. C. Ke, and B. R. Huang. "Properties of coupled surface plasmon-polaritons in metal-dielectric-metal structures." Journal of Applied Physics 112, no. 3 (2012): 033111. http://dx.doi.org/10.1063/1.4745051.

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38

Blonkowski, S., M. Regache, and A. Halimaoui. "Non-linear dielectric properties of metal–amorphous-tantalum pentoxide–metal structures." Journal of Non-Crystalline Solids 303, no. 1 (2002): 108–13. http://dx.doi.org/10.1016/s0022-3093(02)00975-4.

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39

Kashapov, A. I., E. A. Bezus, D. A. Bykov, and L. L. Doskolovich. "Second-order optical differentiator based on a composite metal–dielectric–metal structure." Известия Российской академии наук. Серия физическая 87, no. 1 (2023): 19–24. http://dx.doi.org/10.31857/s036767652270003x.

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Optical properties of a composite structure consisting of two sequentially arranged three-layer metal-dielectric-metal structures (MDM-structures) are considered. It is shown that such a composite MDM-structure can perform second-order spatiotemporal differentiation with high quality at normal incidence. The obtained results can find application in creating systems for analog optical computing and optical information processing.
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40

Ezhovskii, Yu K., and S. V. Mikhailovskii. "Molecular Layering of an Additive Layer of Silicon Dioxide on Anodized Tantalum and Niobium Oxides." Микроэлектроника 53, no. 1 (2024): 85–90. http://dx.doi.org/10.31857/s0544126924010093.

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The results of studying the processes of formation of nanolayers of silicon oxide by the method of molecular layering (atomic layer deposition) on the surface of films of tantalum and niobium oxides obtained by electrochemical oxidation of the corresponding metals are presented. A study of the electrical strength of metal-dielectric-metal (MDM) structures based on tantalum and niobium oxides showed that the introduction of an additive dielectric layer (SiO2) can significantly increase the electrical strength of these structures.
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41

Krutskikh, V. V., A. Yu Sizyakova, M. S. Minkara, A. R. Ibrahim, A. E. Mirzoyan, and A. N. Ushkov. "Broadband Metal-Dielectric Waveguide Path with Low Losses in the EHF Range." Rocket-space device engineering and information systems 8, no. 3 (2021): 89–98. http://dx.doi.org/10.30894/issn2409-0239.2021.8.3.89.98.

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. The present paper is devoted to the design of a new shielded metal-dielectric waveguide with low losses (less than 0.5 dB/m) and wide bandwidth for the 90–100 GHz frequency range. Various types of waveguide structures were analyzed, such as metal waveguides, oversized metal waveguides, dielectric waveguides, dielectric waveguides with a metal shield and various designs of the dielectric filling element. Estimates of loss per unit length in them are obtained. The design of a waveguide containing an oversized round metal screen and a dielectric element consisting of a plate and a rod, located
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42

Ju, Y. “Sungtaek”, Ming-Tsung Hung, and Takane Usui. "Nanoscale Heat Conduction Across Metal-Dielectric Interfaces." Journal of Heat Transfer 128, no. 9 (2006): 919–25. http://dx.doi.org/10.1115/1.2241839.

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We report a theoretical study of heat conduction across metal-dielectric interfaces in devices and structures of practical interest. At cryogenic temperatures, the thermal interface resistance between electrodes and a substrate is responsible for substantial reduction in the maximum permissible peak power in Josephson junctions. The thermal interface resistance is much smaller at elevated temperatures but it still plays a critical role in nanoscale devices and structures, especially nanolaminates that consist of alternating metal and dielectric layers. A theoretical model is developed to eluci
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43

Saeidi, Parviz, Bernhard Jakoby, Gerald Pühringer, et al. "Design, Analysis, and Optimization of a Plasmonic Slot Waveguide for Mid-Infrared Gas Sensing." Nanomaterials 12, no. 10 (2022): 1732. http://dx.doi.org/10.3390/nano12101732.

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In this work, we investigated the optimization of a plasmonic slot waveguide (PSWG) in the mid-IR region particularly for a representative wavelength of 4.26 µm, which is the absorption line of CO2 and thus particularly relevant for applications. We analysed the mode features associated with metal-dielectric-metal (MDM), dielectric-metal-dielectric (DMD), and truncated metal film (TMF) structures with respect to the considered PSWG. Subsequently, the mode features of the PSWG were considered based on what we outlined for MDM, DMD, and TMF structures. Furthermore, as confinement factor and prop
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Mitra, Kalyan Yoti, Enrico Sowade, Christoph Sternkiker, et al. "Investigation on Electrical Stress over Metal-Insulator-Metal (MIM) Structures Based on Compound Dielectrics for the Inkjet-Printed OTFT Stability." Applied Mechanics and Materials 748 (April 2015): 129–33. http://dx.doi.org/10.4028/www.scientific.net/amm.748.129.

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One of the greatest challenges in the field of printed electronics is the performance stability of the devices fabricated by the different printing technologies e.g. inkjet or gravure printing technology. The performance instability can be defined in terms of the device breakdown or by other effects like the emergence of leakage current under the constant high voltage inputs (especially the dielectric within the transistor architecture). The reasons behind this phenomenon can be various, but the most prominent indication can be detected from the materials used and the deposition methodology. F
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Aleshnikov, A. A., Yu E. Kalinin, A. V. Sitnikov, and A. G. Fedosov. "New multilayer structures based on nanogranulated metal-dielectric composites." Bulletin of the Russian Academy of Sciences: Physics 77, no. 10 (2013): 1289–92. http://dx.doi.org/10.3103/s106287381310002x.

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Silva, E., M. Lanucara, and R. Marcon. "The effective surface resistance of superconductor/dielectric/metal structures." Superconductor Science and Technology 9, no. 11 (1996): 934–41. http://dx.doi.org/10.1088/0953-2048/9/11/003.

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Savelev, R. S., I. V. Shadrivov, and Yu S. Kivshar. "Wave scattering by metal-dielectric multilayer structures with gain." JETP Letters 100, no. 11 (2015): 731–36. http://dx.doi.org/10.1134/s002136401423012x.

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Yakymenko, Yurii, Oleksandr Machulianskyi, Bohdan Babych, and Viktor Hetmanchuk. "Metal-Dielectric Nanocomposite Structures with Definite Optical Selective Properties." Radioelectronics and Communications Systems 65, no. 11 (2022): 587–96. http://dx.doi.org/10.3103/s0735272722120044.

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Nesterenko, D. V. "Resonance characteristics of transmissive optical filters based on metal/dielectric/metal structures." Computer Optics 44, no. 2 (2020): 219–28. http://dx.doi.org/10.18287/2412-6179-co-681.

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The resonance characteristics of the Fabry-Pérot resonator modes supported by metal/dielectric/metal planar structures are studied in the case of absorbing media for near-to-normal light incidence. Approximations based on rigorous solution and field-transfer model for the field and resonance line shapes in spectra are attributed to the class of Fano and Lorentz resonances. The analytical expressions are obtained for the propagation constant and field enhancement of the mode, width, height and slope of resonance line shapes in spectra as functions of structural parameters. With estimation of fi
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Avanesyan, V. T., and G. I. Grabko. "Isothermal polarization in thin-film Al-As2Se3-Al metal-dielectric-metal structures." Semiconductors 41, no. 12 (2007): 1419–21. http://dx.doi.org/10.1134/s106378260712007x.

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