Diffraction gratings of isotropic negative-phase velocity materials
Diffraction of electromagnetic plane waves by the gratings made by periodically corrugating the exposed planar boundaries of homogeneous, isotropic, linear dielectric-magnetic half-spaces is examined. The phase velocity vector in the diffracting material can be either co-parallel or anti-parallel to...
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2005
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| LEADER | 11643caa a22011777a 4500 | ||
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| 001 | PAPER-22148 | ||
| 003 | AR-BaUEN | ||
| 005 | 20250221084017.0 | ||
| 008 | 190411s2005 xx ||||fo|||| 00| 0 eng|d | ||
| 024 | 7 | |2 scopus |a 2-s2.0-13944278512 | |
| 040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
| 100 | 1 | |a Depine, Ricardo Angel | |
| 245 | 1 | 0 | |a Diffraction gratings of isotropic negative-phase velocity materials |
| 260 | |c 2005 | ||
| 270 | 1 | 0 | |m Depine, R.A.; Grupo De Electromagnetismo Aplicado, Departamento De Física, Fac. De Cie. Exact. Y Nat., Univ. D., Pabellón I, 1428 Buenos Aires, Argentina; email: rdep@df.uba.ar |
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| 506 | |2 openaire |e Política editorial | ||
| 520 | 3 | |a Diffraction of electromagnetic plane waves by the gratings made by periodically corrugating the exposed planar boundaries of homogeneous, isotropic, linear dielectric-magnetic half-spaces is examined. The phase velocity vector in the diffracting material can be either co-parallel or anti-parallel to the time-averaged Poynting vector, thereby allowing for the material to be classified as of either the positive- or the negative-phase velocity (PPV or NPV) type. Three methods used for analyzing dielectric gratings - the Rayleigh-hypothesis method, a perturbative approach, and the C formalism - are extended here to encompass NPV gratings by a careful consideration of field representation inside the refracting half-space. Corrugations of both symmetric as well as asymmetric shapes are studied, as also the diversity of grating response to the linear polarization states of the incident plane wave. The replacement of PPV grating by its NPV analog affects only nonspecular diffraction efficiencies when the corrugations are shallow, and the effect on specular diffraction efficiencies intensifies as the corrugations deepen. Whether the type of the refracting material is NPV or PPV is shown to affect surface wave propagation as well as resonant excitation of surface waves. © 2005 Elsevier GmbH. All rights reserved. |l eng | |
| 536 | |a Detalles de la financiación: Materials Research Science and Engineering Center, Harvard University | ||
| 536 | |a Detalles de la financiación: 802/OC-AR03-04457 | ||
| 536 | |a Detalles de la financiación: Agencia Nacional de Promoción Científica y Tecnológica | ||
| 536 | |a Detalles de la financiación: Universidad de Buenos Aires | ||
| 536 | |a Detalles de la financiación: Consejo Nacional de Investigaciones Científicas y Técnicas | ||
| 536 | |a Detalles de la financiación: R.A.D. acknowledges financial support from Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET), Agencia Nacional de Promoción Científica y Tecnológica (ANPCYT-BID 802/OC-AR03-04457) and Universidad de Buenos Aires (UBA). A.L. acknowledges partial support from the Penn State Materials Research Science and Engineering Center. | ||
| 593 | |a Grupo De Electromagnetismo Aplicado, Departamento De Física, Fac. De Cie. Exact. Y Nat., Univ. D., Pabellón I, 1428 Buenos Aires, Argentina | ||
| 593 | |a Compl. and Theor. Mat. Sci. Group, Dept. of Eng. Science and Mechanics, Pennsylvania State University, University Park, PA 16802-6812, United States | ||
| 690 | 1 | 0 | |a GRATING |
| 690 | 1 | 0 | |a NEGATIVE-PHASE VELOCITY |
| 690 | 1 | 0 | |a NONSPECULAR DIFFRACTION |
| 690 | 1 | 0 | |a NUMERICAL TECHNIQUES |
| 690 | 1 | 0 | |a SURFACE WAVES |
| 690 | 1 | 0 | |a BOUNDARY VALUE PROBLEMS |
| 690 | 1 | 0 | |a DIELECTRIC DEVICES |
| 690 | 1 | 0 | |a ELECTROMAGNETISM |
| 690 | 1 | 0 | |a IMAGE ANALYSIS |
| 690 | 1 | 0 | |a LENSES |
| 690 | 1 | 0 | |a LIGHT POLARIZATION |
| 690 | 1 | 0 | |a LIGHT REFLECTION |
| 690 | 1 | 0 | |a LIGHT REFRACTION |
| 690 | 1 | 0 | |a MAGNETIC MATERIALS |
| 690 | 1 | 0 | |a MAXWELL EQUATIONS |
| 690 | 1 | 0 | |a OPTICS |
| 690 | 1 | 0 | |a PERTURBATION TECHNIQUES |
| 690 | 1 | 0 | |a SURFACE WAVES |
| 690 | 1 | 0 | |a VECTORS |
| 690 | 1 | 0 | |a HELMHOLTZ EQUATIONS |
| 690 | 1 | 0 | |a II |
| 690 | 1 | 0 | |a NEGATIVE-PHASE VELOCITY MATERIALS |
| 690 | 1 | 0 | |a NONSPECULAR DIFFRACTION |
| 690 | 1 | 0 | |a NUMERICAL TECHNIQUES |
| 690 | 1 | 0 | |a DIFFRACTION GRATINGS |
| 700 | 1 | |a Lakhtakia, A. | |
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