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Journal articles on the topic 'Magnetodielectric spheres'

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Author: Grafiati

Published: 30 May 2022

Last updated: 31 May 2022

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1

Kozar, A. I. "Electromagnetic Wave Scattering in a Waveguide Containing Homogeneous Magnetodielectric Spheres." Telecommunications and Radio Engineering 60, no. 7-9 (2003): 11–22. http://dx.doi.org/10.1615/telecomradeng.v60.i789.20.

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2

Kozar, A. I. "Electromagnetic Wave Scattering with Special Spatial Lattices of Magnetodielectric Spheres." Telecommunications and Radio Engineering 61, no. 7-12 (2004): 734–49. http://dx.doi.org/10.1615/telecomradeng.v61.i9.20.

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3

Kozar, A. I. "ELECTROMAGNETIC LATTICE "INVISIBILITY" OF THE RESONANCE CUBIC CRYSTAL MADE OF MAGNETODIELECTRIC SPHERES." Telecommunications and Radio Engineering 77, no. 2 (2018): 155–60. http://dx.doi.org/10.1615/telecomradeng.v77.i2.60.

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4

Liu, Xing-Xiang, and Andrea Alù. "Homogenization of quasi-isotropic metamaterials composed by dense arrays of magnetodielectric spheres." Metamaterials 5, no. 2-3 (June 2011): 56–63. http://dx.doi.org/10.1016/j.metmat.2011.04.001.

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5

Shore, R. A., and A. D. Yaghjian. "Traveling Waves on Three-Dimensional Periodic Arrays of Two Different Alternating Magnetodielectric Spheres." IEEE Transactions on Antennas and Propagation 57, no. 10 (October 2009): 3077–91. http://dx.doi.org/10.1109/tap.2009.2024495.

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6

Kozar, A. I. "Structural Function Development for Electromagnetic Interactions in the System of Multiple Resonant Magnetodielectric Spheres." Telecommunications and Radio Engineering 63, no. 7 (2005): 589–605. http://dx.doi.org/10.1615/telecomradeng.v63.i7.20.

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7

Kozar, A. I. "Figurate Numbers (Arithmetic Progression) and Electromagnetic Wave Scattering on Spatial Lattices of Resonant Magnetodielectric Spheres." Telecommunications and Radio Engineering 59, no. 7-9 (2003): 11. http://dx.doi.org/10.1615/telecomradeng.v59.i7-9.30.

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8

Kozar, A. I. "Structure Functions of Electromagnetic Field Coupling in a Cavity Filled by Resonance-Size Magnetodielectric Spheres." Telecommunications and Radio Engineering 61, no. 5 (2004): 363–81. http://dx.doi.org/10.1615/telecomradeng.v61.i5.10.

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9

Auñón, Juan Miguel, and Manuel Nieto-Vesperinas. "Optical forces from evanescent Bessel beams, multiple reflections, and Kerker conditions in magnetodielectric spheres and cylinders." Journal of the Optical Society of America A 31, no. 9 (August 14, 2014): 1984. http://dx.doi.org/10.1364/josaa.31.001984.

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10

Liu, Jin, and Nicola Bowler. "Analysis of losses in a double-negative metamaterial composed of magnetodielectric spheres embedded in a matrix." Microwave and Optical Technology Letters 53, no. 7 (April 22, 2011): 1649–52. http://dx.doi.org/10.1002/mop.26081.

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11

Kozar, A. I. "Scattering of electromagnetic waves by a discrete octahedron from resonant spheres." Radiotekhnika, no. 203 (December 23, 2020): 181–85. http://dx.doi.org/10.30837/rt.2020.4.203.19.

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A solution is given to the problem of scattering of electromagnetic waves by a discrete convex polyhedron – an octahedron of resonant magnetodielectric spheres based on a complex rhombic crystal lattice. Here we consider a case equivalent to the X-ray optics of crystals, when α / λ՛<<1 and can be α / λg ~ 1; d, h, l / λ՛ ~ 1, where α is the radius of the spheres; λ՛, λg are the lengths of the scattered wave outside and inside the spheres; d, h, l are constant lattices. The solution of the problem is obtained based on the Fredholm integral equations of electrodynamics of the second kind with nonlocal boundary conditions. The expressions found in this work for a metacrystal in the form of an octahedron can be used to study the fields scattered by the crystal in the Fresnel and Fraunhofer zones, as well as to study its internal field. The relations obtained in this work can find application in the study of the scattering of waves of various kinds by convex polyhedrons, the creation on their basis of new types of limited metacrystals, including nanocrystals with resonance properties, and in the study of their behavior in various external media. As well as in the development of methods for modeling electromagnetic phenomena that can occur in real crystals in resonance regions in the optical and X-ray wavelength ranges.

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12

Jin Liu and Nicola Bowler. "Analysis of Double-Negative (DNG) Bandwidth for a Metamaterial Composed of Magnetodielectric Spheres Embedded in a Matrix." IEEE Antennas and Wireless Propagation Letters 10 (2011): 399–402. http://dx.doi.org/10.1109/lawp.2011.2150191.

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13

Li, Yang, and Robert A. Shore. "Corrections to “Traveling Waves on Three-Dimensional Periodic Arrays of Two Different Alternating Magnetodielectric Spheres” [Oct 09 3077-3091]." IEEE Transactions on Antennas and Propagation 59, no. 7 (July 2011): 2753–54. http://dx.doi.org/10.1109/tap.2011.2152355.

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14

Li, Yang, and Nicola Bowler. "Traveling Waves on Three-Dimensional Periodic Arrays of Two Different Magnetodielectric Spheres Arbitrarily Arranged on a Simple Tetragonal Lattice." IEEE Transactions on Antennas and Propagation 60, no. 6 (June 2012): 2727–39. http://dx.doi.org/10.1109/tap.2012.2194637.

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15

Li, Yang, and Nicola Bowler. "Analysis of Double-Negative (DNG) Bandwidths for Metamaterials Composed of Three-Dimensional Periodic Arrays of Two Different Magnetodielectric Spheres Arbitrarily Arranged on a Simple Tetragonal Lattice." IEEE Antennas and Wireless Propagation Letters 10 (2011): 1484–87. http://dx.doi.org/10.1109/lawp.2011.2179970.

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16

TEO, L. P. "MODE SUMMATION APPROACH TO CASIMIR EFFECT BETWEEN TWO OBJECTS." International Journal of Modern Physics A 27, no. 25 (October 10, 2012): 1230021. http://dx.doi.org/10.1142/s0217751x12300219.

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In the last few years, several approaches have been developed to compute the exact Casimir interaction energy between two nonplanar objects, all lead to the same functional form, which is called the TGTG formula. In this paper, we explore the TGTG formula from the perspective of mode summation approach. Both scalar fields and electromagnetic fields are considered. In this approach, one has to first solve the equation of motion to find a wave basis for each object. The two T's in the TGTG formula are [Formula: see text]-matrices representing the Lippmann–Schwinger T-operators, one for each of the objects. Each [Formula: see text]-matrix can be found by matching the boundary conditions imposed on the object, and it is independent of the other object. However, it depends on whether the object is interacting with an object outside it, or an object inside it. The two G's in the TGTG formula are the translation matrices, relating the wave basis of an object to the wave basis of the other object. These translation matrices only depend on the wave basis chosen for each object, and they are independent of the boundary conditions on the objects. After discussing the general theory, we apply the prescription to derive the explicit formulas for the Casimir energies for the sphere–sphere, sphere–plane, cylinder–cylinder and cylinder–plane interactions. First the [Formula: see text]-matrices for a plane, a sphere and a cylinder are derived for the following cases: the object is imposed with Dirichlet, Neumann or general Robin boundary conditions; the object is semitransparent; and the object is a magnetodielectric object immersed in a magnetodielectric media. Then the operator approach developed by R. C. Wittman [IEEE Trans. Antennas Propag.36, 1078 (1988)] is used to derive the translation matrices. From these, the explicit TGTG formula for each of the scenarios can be written down. On the one hand, we have summarized all the TGTG formulas that have been derived so far for the sphere–sphere, cylinder–cylinder, sphere–plane and cylinder–plane configurations. On the other hand, we provide the TGTG formulas for some scenarios that have not been considered before.

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17

Kozar, Anatoliy. "Electromagnetic lattice "invisibility" of the photon crystal made of magnetodielectric spheres in the form of octahedron." Eskişehir Technical University Journal of Science and Technology A - Applied Sciences and Engineering, December 16, 2019. http://dx.doi.org/10.18038/estubtda.652363.

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18

Abbasi, Farah R., Z. A. Awan, and Arshad Hussain. "Backscattering cross-section from a metamaterial coated sphere covered with a metasurface." International Journal of Microwave and Wireless Technologies, April 22, 2021, 1–11. http://dx.doi.org/10.1017/s1759078721000581.

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Abstract An analysis about the backscattering characteristics of a metamaterial coated magnetodielectric sphere covered with a metasurface has been presented. The effects of various types of metamaterial coatings and surface reactances of lossless metasurface upon the backscattering cross-section of a metamaterial coated magnetodielectric sphere covered with a metasurface have been studied. It is shown that the negligible backscattering cross-section from a double near-zero metamaterial coated magnetodielectric sphere can be enhanced significantly by using specific types of lossless metasurfaces. These types of enhanced backscattering cross-section find applications in the radar detection problems. The proposed theory is also extended to the lossy double negative metamaterial coated magnetodielectric sphere covered with a lossless metasurface. During the study, it is found that for a specific part of the lossy double negative metamaterial bandwidth, two specific types of lossless metasurfaces can be used to reduce the backscattering cross-section as compared to the backscattering cross-section of a lossy double negative metamaterial coated magnetodielectric sphere without metasurface.

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19

Sambale, Agnes, Stefan Yoshi Buhmann, and Stefan Scheel. "Casimir-Polder interaction between an atom and a small magnetodielectric sphere." Physical Review A 81, no. 1 (January 28, 2010). http://dx.doi.org/10.1103/physreva.81.012509.

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