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Artykuły w czasopismach na temat „Transverse electric”

Autor: Grafiati

Data publikacji: 3 czerwca 2025

Data aktualizacji: 31 lipca 2025

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1

Fadeyeva, T. A. "Singular beams with transverse electric and transverse magnetic fields." Semiconductor Physics Quantum Electronics and Optoelectronics 16, no. 1 (2013): 55–58. http://dx.doi.org/10.15407/spqeo16.01.055.

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2

ZHOU, BIN, and SHUN-QING SHEN. "SPIN TRANSVERSE FORCE AND QUANTUM TRANSVERSE TRANSPORT." International Journal of Modern Physics B 22, no. 01n02 (2008): 76–81. http://dx.doi.org/10.1142/s0217979208046074.

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We present a brief review on spin transverse force, which exerts on the spin as the electron is moving in an electric field. This force, analogue to the Lorentz force on electron charge, is perpendicular to the electric field and spin current carried by the electron. The force stems from the spin-orbit coupling of electrons as a relativistic quantum effect, and could be used to understand the Zitterbewegung of electron wave packet and the quantum transverse transport of electron in a heuristic way.

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3

Shvartsburg, A. B., L. Stenflo, and P. K. Shukla. "Transverse-electric polarized surface solitons." Physics Letters A 268, no. 4-6 (2000): 386–89. http://dx.doi.org/10.1016/s0375-9601(00)00190-0.

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4

Gevorkyan E. A. "Transverse components of the electromagnetic field in a waveguide with modulated in space and in time magnetodielectric filling." Optics and Spectroscopy 130, no. 10 (2022): 1293. http://dx.doi.org/10.21883/eos.2022.10.54865.3813-22.

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The propagation of transverse magnetic (TM) and transverse electric (TE) electromagnetic waves in a regular ideal waveguide of arbitrary cross section is considered. It is assumed that the permittivity and permeability of the magnetodielectric filling of the waveguide are functions that depend on the coordinate and time. Analytical expressions for the transverse components of the magnetic and electric vectors of the TM- and TE-fields in the waveguide are obtained from the system of Maxwell equations. They are expressed in terms of the longitudinal components of the electric and magnetic vector

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5

Lee, Sung Uk, Hyo Joon Eom, Jang Soo Ock, and Jong Hwa Kwon. "Higher-Order Transverse Electric and Transverse Magnetic Modes in Gigahertz Transverse Electromagnetic Cells." Electromagnetics 31, no. 7 (2011): 483–93. http://dx.doi.org/10.1080/02726343.2011.607104.

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6

Preethichandra, D. M. G. "An Experimental Investigation on Polypyrrole Films Electro-Polymerized under a High Transverse Electric Field." Applied Mechanics and Materials 343 (July 2013): 77–83. http://dx.doi.org/10.4028/www.scientific.net/amm.343.77.

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Polypyrrole films were electrodeposited under different high transverse electric fields, and their film morphologies and functionalities were investigated. The surface morphology at the initial polymerization stage was investigated under AFM and the cross sectional morphologies of fully grown films were investigated by SEM. Both these microscopic investigations revealed the film morphology has been influenced by the applied transverse field. The cyclic voltammetry tests illustrate a reduction in the anodic peak voltage with the increase of transverse field. All these results suggest that the p

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7

Bautista-Anguiano, Joshua C., and Teruhiko Hagiwara. "Bed-Detection Sensitivity Employing 1D Response to an Electric Dipole Source in Multilayer Anisotropic Formations." Petrophysics – The SPWLA Journal of Formation Evaluation and Reservoir Description 63, no. 4 (2022): 519–33. http://dx.doi.org/10.30632/pjv63n4-2022a3.

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Electric and magnetic field responses originating from a primary electric current source have been analytically derived, explored, and employed to explore and detect electrical anomalies due to the presence of a bed boundary in a two-layer model, using the controlled source electromagnetic method. However, previous works on the subject demand in-depth knowledge of mathematics, which could become an obstacle for the practitioner looking to immerse into the realm of induction logging and who needs a straightforward approach to develop their algorithms. Consequently, we introduce the analytical e

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8

Warber, C. R., and E. C. Field. "A long wave transverse electric-transverse magnetic noise prediction model." Radio Science 30, no. 3 (1995): 783–97. http://dx.doi.org/10.1029/94rs03181.

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9

McCutcheon, Murray W., Parag B. Deotare, Yinan Zhang, and Marko Lončar. "High-Q transverse-electric/transverse-magnetic photonic crystal nanobeam cavities." Applied Physics Letters 98, no. 11 (2011): 111117. http://dx.doi.org/10.1063/1.3568897.

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10

Boardman, A. D., and T. Twardowski. "Transverse-electric and transverse-magnetic waves in nonlinear isotropic waveguides." Physical Review A 39, no. 5 (1989): 2481–92. http://dx.doi.org/10.1103/physreva.39.2481.

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11

Ghezali, S., and M. Slimani. "Transverse magnetic mode excitation in an atomic mirror." Physics & Astronomy International Journal 6, no. 4 (2022): 156–60. http://dx.doi.org/10.15406/paij.2022.06.00269.

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We present a study of a transverse magnetic mode excitation in a multi-layer atomic mirror. We give the continuity relationships at the interfaces of the setting.1 We deduce the transverse and parallel components of the electric field through the atomic mirror and then the total component. We show that there is no enhancement of the electric field in the vaccum contrarily to the transverse electric field excitation.2

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12

Chen, Rui-Pin, and Khian-Hooi Chew. "Far-field properties of a vortex Airy beam." Laser and Particle Beams 31, no. 1 (2012): 9–15. http://dx.doi.org/10.1017/s0263034612000729.

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AbstractAnalytical far-field expressions for the transverse electric mode and transverse electric magnetic mode terms, and the energy flux distributions of vortex Airy beams are derived based on the vector angular spectrum of the beam and the stationary phase method. The physical pictures of vortex Airy beams from the vectorial structure are illustrated and the energy flux distributions are demonstrated in far-field. The influences of the beam parameters, especially the exponential factor, on the energy flux distributions of vortex Airy beams and its transverse electric mode and transverse ele

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13

Логинов, Д. К., та А. В. Донец. "Зависимость продольно-поперечного расщепления экситона в квантовой яме от внешнего однородного электрического поля". Физика твердого тела 62, № 2 (2020): 208. http://dx.doi.org/10.21883/ftt.2020.02.48869.599.

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In our paper theoretical analyzed the decreasing of transverse-longitudinal splitting of an exciton in the GaAs/AlGaAs quantum well in the homogeneous electric field. Also the dependence of the splitting on application field is calculated. The excitonic reflectance spectra of the thick quantum well are calculated for field directed transversal to well layer. The decreasing of reflectance oscillation in the excitonic spectra because of decreasing transverse-longitudinal splitting is demonstrated.

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14

Siew, Y. H., and J. E. Aubrey. "The transverse electric fields in zinc." Journal of Physics D: Applied Physics 18, no. 9 (1985): 1735–43. http://dx.doi.org/10.1088/0022-3727/18/9/005.

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15

Jablan, Marinko, Hrvoje Buljan, and Marin Soljačić. "Transverse electric plasmons in bilayer graphene." Optics Express 19, no. 12 (2011): 11236. http://dx.doi.org/10.1364/oe.19.011236.

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16

Lipavský, P., J. Koláček, and P. J. Lin. "Transverse acousto-electric effect in superconductors." Physica C: Superconductivity and its Applications 525-526 (June 2016): 10–17. http://dx.doi.org/10.1016/j.physc.2016.03.012.

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17

Aubrey, J. E., G. P. Yick, and D. I. Westwood. "Transverse electric fields in n-GaAs." Electronics Letters 28, no. 4 (1992): 432. http://dx.doi.org/10.1049/el:19920271.

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18

Sheppard, C. J. R., and S. Saghafi. "Transverse-electric and transverse-magnetic beam modes beyond the paraxial approximation." Optics Letters 24, no. 22 (1999): 1543. http://dx.doi.org/10.1364/ol.24.001543.

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19

Ye, Hui, and Jeffrey Ng. "Shielding effects of myelin sheath on axolemma depolarization under transverse electric field stimulation." PeerJ 6 (December 3, 2018): e6020. http://dx.doi.org/10.7717/peerj.6020.

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Axonal stimulation with electric currents is an effective method for controlling neural activity. An electric field parallel to the axon is widely accepted as the predominant component in the activation of an axon. However, recent studies indicate that the transverse component to the axolemma is also effective in depolarizing the axon. To quantitatively investigate the amount of axolemma polarization induced by a transverse electric field, we computed the transmembrane potential (Vm) for a conductive body that represents an unmyelinated axon (or the bare axon between the myelin sheath in a mye

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20

Liu, Jian, Xin Wang, Shu Mao Wang, and Han Fu. "The Structure Design of Low Frequency Electromagnetic Induction Heating System Based on Analysis of Thermal Effect." Applied Mechanics and Materials 433-435 (October 2013): 1549–53. http://dx.doi.org/10.4028/www.scientific.net/amm.433-435.1549.

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The low frequency transverse magnetic electric induction heating system uses high penetration of low frequency electromagnetic induction heat objects, which is new and high efficient. Due to the magnetic fluxing through objects transversely, it is different with other electromagnetic induction heating methods and this makes it applied more widely. And in this paper, we present the application of low frequency transverse magnetic electric induction heating system in the technique of the lock temperature on seamless line. With the analysis of heating efficiency, it also combines the theory of ed

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21

Klimchitskaya, Galina L., and Vladimir M. Mostepanenko. "Casimir Effect Invalidates the Drude Model for Transverse Electric Evanescent Waves." Physics 5, no. 4 (2023): 952–67. http://dx.doi.org/10.3390/physics5040062.

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We consider the Casimir pressure between two metallic plates and calculate the four contributions to it determined by the propagating and evanescent waves and by the transverse magnetic and transverse electric polarizations of the electromagnetic field. The range of interplate separations is considered where nearly the whole pressure has its origin in the electromagnetic response of conduction electrons. In the Casimir physics, this response is described either by the dissipative Drude model resulting in contradictions with the measurement data or by the experimentally consistent but dissipati

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22

Ouchani, Noama, Driss Bria, Bahram Djafari-Rouhani, and Abdelkarim Nougaoui. "Transverse-electric/transverse-magnetic polarization converter using 1D finite biaxial photonic crystal." Journal of the Optical Society of America A 24, no. 9 (2007): 2710. http://dx.doi.org/10.1364/josaa.24.002710.

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23

Latyshev, A. V., and A. A. Yushkanov. "Transverse electric conductivity in collisional quantum plasma." Plasma Physics Reports 38, no. 11 (2012): 899–908. http://dx.doi.org/10.1134/s1063780x12100078.

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24

Jiang, Yi, Mei Kong, Can Liu, Yao Liu, and Yu Wang. "Transverse electric modes in planar slot waveguides." Journal of Modern Optics 65, no. 1 (2017): 111–18. http://dx.doi.org/10.1080/09500340.2017.1377307.

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25

S̆imánek, E. "Transverse electric fields in mesoscopic normal rings." Physics Letters A 250, no. 4-6 (1998): 425–29. http://dx.doi.org/10.1016/s0375-9601(98)00759-2.

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26

Ukhtary, M. Shoufie, Ahmad R. T. Nugraha, Eddwi H. Hasdeo, and Riichiro Saito. "Broadband transverse electric surface wave in silicene." Applied Physics Letters 109, no. 6 (2016): 063103. http://dx.doi.org/10.1063/1.4960531.

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27

Montambaux, Gilles. "Density waves in a transverse electric field." Physical Review B 54, no. 24 (1996): R17273—R17275. http://dx.doi.org/10.1103/physrevb.54.r17273.

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28

Tsitsos, S., and A. A. P. Gibson. "Transverse electric modes in shielded strip line." Microwave and Optical Technology Letters 7, no. 10 (1994): 438–40. http://dx.doi.org/10.1002/mop.4650071004.

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29

Asma, Mohammed Elbashir Saad*1 Mubarak Dirar Abdallah2 &. Swsan Ahmed Elhouri Ahmed3. "TIME DEPENDENT SCHRÖDINGER EQUATION FOR TWO LEVEL SYSTEMS TO FIND TRAVERSE RELAXATION TIME." GLOBAL JOURNAL OF ENGINEERING SCIENCE AND RESEARCHES 6, no. 3 (2019): 251–62. https://doi.org/10.5281/zenodo.2616917.

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Transverse relaxation time is important in magnetic resonance imaging (MRI). It is important to construct new models to find new parameters that control imaging quality. In this work Schrodinger Equation in energy space for two level systems was used to find transverse relaxation time.  By suggesting sine and cosine beside complex solutions a useful expression for transverse relaxation time was found. When electric interaction dominate, i.e. for dielectric materials the transverse relaxation time depends on the electric dipole moment. However the magnetic materials having magnetic spin an

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30

Yusupbekov, N. R., та N. M. Zakhidov. "ФОТОЭЛЕКТРИЧЕСКИЙ СТВОРОФИКСАТОР С ОПТИКО-ЭЛЕКТРОННЫМ АНАЛИЗАТОРОМ". Journal of Science and Innovative Development 6, № 2 (2023): 53–61. http://dx.doi.org/10.36522/2181-9637-2023-2-6.

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The article discusses a technical solution for improvement of alignment measurement tools by means of a laser beam as a reference baseline and photoelectrical recorder of high accuracy, wide range and capacity. It also provides a brief review of classifications of modern primary transducers of alignment measurements which forms the basis for a patented design and an electronic block diagram of a photoelectric alignment fixer with an opto-electronic analyzer. The proposed device, in contrast to modern analogs, has small weight and size parameters and provides high efficiency of retrieval of dat

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31

Tarkhanyan, Roland H., and Dimitris G. Niarchos. "Geometrically Tunable Transverse Electric Field in Multilayered Structures." Advances in Condensed Matter Physics 2017 (2017): 1–4. http://dx.doi.org/10.1155/2017/1216867.

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Appearance of a transverse component in dc electric field with respect to the applied current is investigated in periodic multilayer composite structures made of nanometer-to-micrometer scale alternating layers of two different homogeneous and isotropic conducting materials. Dependence of the transverse electric field on geometrical orientation of the layers is examined using the coordinate transformation approach. Electric field bending angle as a function of the layers’ resistivity ratio is studied in detail. It is shown that both the direction and the magnitude of the field can be changed u

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32

Zhao, Ke, Xiao Min Lei, Guo Feng Xie, and Wen Hua Xiong. "Research of High Performance Polarization-Independent Grating Beam Splitter." Applied Mechanics and Materials 310 (February 2013): 481–85. http://dx.doi.org/10.4028/www.scientific.net/amm.310.481.

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Based on a silicon-on-insulator (Silicon-on-insulator, SOI) material system design and optimization of a high performance, the polarization independent of 1 × 3 subwavelength grating stars beam splitter. By a rigorous coupled-wave analysis method showed that, in the 1550nm wavelength range, at vertical incidence, the device on the transverse electric field (transverse electric, TE) ,the 0 and ± 1 order transmittance is 31%, 32%, 32%,respectively; cross the magnetic field (transverse magnetic, TM), the 0 and ± 1 transmittance is 33%, 32%, 32%, respectively.

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33

Minhas, Dr S. S., Dr J. K. Mahajan, and Dr D. C. Merwaha. "Extensive Abdominal Electric Burn Injury." Indian Journal of Plastic Surgery 24, no. 02 (1991): 034–35. http://dx.doi.org/10.1055/s-0043-1775696.

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34

Chiang (Tszyan), Yu N., and M. O. Dzyuba. "Transverse spin effects in electron transport." Low Temperature Physics 49, no. 1 (2023): 136–44. http://dx.doi.org/10.1063/10.0016487.

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In the samples of nonmagnetic Al, Pt, and W metals of an asymmetric shape, which causes a nonequilibrium distribution of charge carriers, the transverse spin contributions of the spin-orbit interaction to the Hall and Nernst-Ettingshausen effects were studied by direct electric measurement. It is found a difference in the behavior of the spin contributions of thermal diffusion and electric nature in a magnetic field. The dependence of this behavior on the band structure that controls the profiles of spin magnetization, which is established at the edges of the sample by the accumulation of spin

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35

Emir, Recep, Cagatay Tuncsiper, Dilek Surekci Yamacli, Serhan Yamacli, and Sezai Alper Tekin. "Investigation of Electric Field Tunable Optical and Electrical Characteristics of Zigzag and Armchair Graphene Nanoribbons: An Ab Initio Approach." Nanomaterials 14, no. 17 (2024): 1446. http://dx.doi.org/10.3390/nano14171446.

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Graphene nanoribbons (GNRs), categorized into zigzag and armchair types, hold significant promise in electronics due to their unique properties. In this study, optical properties of zigzag and armchair GNRs are investigated using density functional theory (DFT) in conjunction with Kubo–Greenwood formalism. Our findings reveal that optical characteristics of both GNR types can be extensively modulated through the application of a transverse electric field, e.g., the refractive index of the a zigzag GNR is shown to vary in the range of n = 0.3 and n = 9.9 for the transverse electric field values

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36

Wu, Qifeng, Cunrui Bo, Kaixiang Sun, and Liangbi Li. "Redistribution of Residual Stresses in Titanium Alloy Butt-Welded Thick Plates Due to Wire-Cut Electrical Discharge Machining." Metals 15, no. 7 (2025): 750. https://doi.org/10.3390/met15070750.

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Welding and cutting behaviour may affect the mechanical properties of titanium alloy welded structures, which may have some impact on the safety assessment of the structure. This study analyses changes in residual stress in Ti80 butt-welded thick plates before and after wire-cut electric discharge machining, using numerical simulations based on thermo-elastoplastic theory and the element birth and death method, validated by X-ray non-destructive testing. The transverse residual tensile stress near the weld exhibits an asymmetric bimodal distribution, while the longitudinal stress is significan

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37

Kołacz, Jakub, Henry G. Gotjen, Robel Y. Bekele, et al. "Propagating transverse electric and transverse magnetic modes in liquid crystal-clad planar waveguides." Liquid Crystals 47, no. 4 (2019): 531–39. http://dx.doi.org/10.1080/02678292.2019.1662110.

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38

Melamed, Timor, Dor Abuhasira, and David Dayan. "Transverse electric and transverse magnetic pulsed-beam decomposition of time-dependent aperture fields." Journal of the Optical Society of America A 29, no. 6 (2012): 1115. http://dx.doi.org/10.1364/josaa.29.001115.

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39

Valovik, Dmitry V. "On the problem of nonlinear coupled electromagnetic transverse-electric–transverse magnetic wave propagation." Journal of Mathematical Physics 54, no. 4 (2013): 042902. http://dx.doi.org/10.1063/1.4799275.

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40

Gómez-Díaz, J. S., and J. Perruisseau-Carrier. "Propagation of hybrid transverse magnetic-transverse electric plasmons on magnetically biased graphene sheets." Journal of Applied Physics 112, no. 12 (2012): 124906. http://dx.doi.org/10.1063/1.4769749.

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41

Raafat, Hazem. "Reconstruction of multilayered dielectric models using oblique transverse electric or transverse magnetic incidence." Optical Engineering 34, no. 4 (1995): 1172. http://dx.doi.org/10.1117/12.196460.

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42

Theuer, M., A. J. Shutler, S. Sree Harsha, R. Beigang, and D. Grischkowsky. "Terahertz two-cylinder waveguide coupler for transverse-magnetic and transverse-electric mode operation." Applied Physics Letters 98, no. 7 (2011): 071108. http://dx.doi.org/10.1063/1.3554761.

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43

Zhao, Chunwang, Yannan Xue, and Yongjun Jin. "Effect of electric field on Fe2O3 nanowire growth during thermal oxidation." Modern Physics Letters B 30, no. 06 (2016): 1650054. http://dx.doi.org/10.1142/s0217984916500548.

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A direct current of 5 A was applied to narrow strips of iron foil in air to synthesize iron oxide nanowires (NWs) via thermal oxidation route of resistive heating. Transverse electric fields of 0–4000 V/m were applied perpendicularly to the surface of the iron foil during thermal oxidations. Results showed that the Fe2O3 NW array can grow perpendicularly on that surface by using this kind of thermal oxidation method. Transverse electric fields applied during thermal oxidation significantly affected the morphology of the Fe2O3 NW array. With increasing strength of the transverse electric fields

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44

Belubekyan, M. V., S. V. Sargsyan, and A. A. Papyan. "LOCALIZED BENDING VIBRATIONS OF PIEZOCERAMIC TRANSVERSE POLARIZED PLATE." Proceedings of the YSU A: Physical and Mathematical Sciences 52, no. 1 (245) (2018): 27–33. http://dx.doi.org/10.46991/pysu:a/2018.52.1.027.

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Problem of the piezoceramic plate polarized along the normal of the middle plane of the plate is solved, based on the assumptions of the hypothesis of Kirchhoff, taking into account the components characterizing the electric field. The equations of planar and bending vibrations are obtained. Localized bending vibrations are considered, and the effect of the electric field on the frequency of localized vibrations is investigated.

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45

Kucherenko, M. G. "MODELING OF CONFORMATIONAL CHANGES OF POLYELECTROLYTES ON THE SURFACE OF A TRANSVERSELY POLARIZED METAL NANOWIRE IN AN EXTERNAL ELECTRIC FIELD." Eurasian Physical Technical Journal 19, no. 2 (40) (2022): 19–29. http://dx.doi.org/10.31489/2022no2/19-29.

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Gold nanowires with polyelectrolytes adsorbed on their surface are widely used in various biomedical research. In this work, for the first time, conformationalchanges in polyelectrolytes on the surface of a gold nanowire transversely polarized in an external electric field were considered. The properties of a specially created analytical model of conformational rearrangements of a Gaussian macromolecular chain adsorbed on the surface of a cylindrical metal nanowire in an external electric field transverse to the axis of the nanowire were investigated. Conformational changes of uniformly charge

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46

Zhang, Haiping, Zhifeng Zeng, and Yong Wang. "Tellurium Photonic Crystal-Based Terahertz Polarization Splitter Using a Diamond-Shaped Ferrite Pillar Array." Crystals 14, no. 12 (2024): 1015. http://dx.doi.org/10.3390/cryst14121015.

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A T-shaped photonic crystal waveguide was designed with square lattice tellurium photonic crystals. A diamond-shaped ferrite pillar array was inserted in the junction of the waveguide to make a novel terahertz polarization splitter. Both transverse electric and transverse magnetic modes were numerically investigated by the plane wave expansion method, which used complete photonic band gaps covering from 0.138 THz to 0.144 THz. In this frequency domain of the fully polarized band gaps, the transmission efficiency of the photonic crystal waveguide was up to −0.21 dB and −1.67 dB for the transver

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47

Hidayat, M. Reza, Mohamad Hamzah Zamzam, and Salita Ulitia Prini. "Excitation Analysis of Transverse Electric Mode Rectangular Waveguide." Jurnal Elektronika dan Telekomunikasi 20, no. 1 (2020): 1. http://dx.doi.org/10.14203/jet.v20.1-8.

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A waveguide is a transmission medium in the form of a pipe and is made from a single conductor. A waveguide has the function of delivering electromagnetic waves with a frequency of 300 MHz - 300 GHz and is able to direct the waves in a particular direction. In its development, a waveguide can be used as a filter. A filter consists of several circuits designed to pass signals that are generated at a specific frequency and attenuate undesired signals. One type of filter that can pass a signal in a particular frequency range and block signals that are not included in that frequency range is a ban

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48

Deng, Ye, Su Xu, Runren Zhang, et al. "Ultra-broadband carpet cloak for transverse-electric polarization." Journal of Optics 18, no. 4 (2016): 044006. http://dx.doi.org/10.1088/2040-8978/18/4/044006.

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Mitha, Tanzeela, and Maria Pour. "Wideband Microstrip Patch Antennas with Transverse Electric Modes." Applied Computational Electromagnetics Society 35, no. 8 (2020): 971–74. http://dx.doi.org/10.47037/2020.aces.j.350817.

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Streszczenie:

A wideband microstrip patch antenna, exciting the fundamental transverse electric (TE) mode, is investigated. The excitation of the TE mode is facilitated through replacing both of the patch and ground plane of a conventional microstrip antenna with artificial magnetic conductors (AMC), consisting of unipolar compact photonic bandgap (UC-PBG) unit cells. The AMC patch and the ground plane of this antenna behave as magnetic conductors within the bandgap region of the unit cells. Similar to conventional patch antennas, it is shown that by cutting a U-shaped slot in the AMC patch, wideband charac

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Hayashi, M., and H. Yoshioka. "Charge density wave in a transverse electric field." Le Journal de Physique IV 09, PR10 (1999): Pr10–145—Pr10–147. http://dx.doi.org/10.1051/jp4:19991036.

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