Application of the differential method to uniaxial gratings with an infinite number of refraction channels: Scalar case
The differential method (also called the C method) is applied to the diffraction of linearly polarized plane waves at a periodically corrugated boundary between vacuum and a linear, homogeneous, uniaxial, dielectric-magnetic medium characterized by hyperbolic dispersion equations. Numerical results...
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2006
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001 | PAPER-7310 | ||
003 | AR-BaUEN | ||
005 | 20250221083544.0 | ||
008 | 190411s2006 xx ||||fo|||| 00| 0 eng|d | ||
024 | 7 | |2 scopus |a 2-s2.0-29344439108 | |
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100 | 1 | |a Depine, Ricardo Angel | |
245 | 1 | 0 | |a Application of the differential method to uniaxial gratings with an infinite number of refraction channels: Scalar case |
260 | |c 2006 | ||
270 | 1 | 0 | |m Depine, R.A.; Grupo de Electromagnetismo Aplicado, Departamento de Física, Pabellón I, 1428 Buenos Aires, Argentina; email: rdep@df.uba.ar |
504 | |a Shelby, R.A., Smith, D.R., Schultz, S., (2001) Science, 292, p. 77 | ||
504 | |a Lakhtakia, A., McCall, M.W., Weiglhofer, W.S., (2003) Introduction to Complex Mediums for Optics and Electromagnetics, p. 347. , W.S. Weiglhofer A. Lakhtakia SPIE Press Bellingham, WA, USA | ||
504 | |a MacKay, T.G., Lakhtakia, A., (2004) Phys. Rev. e, 69, p. 026602 | ||
504 | |a Pendry, J.B., Smith, D.R., (2004) Phys. Today, 57, p. 37 | ||
504 | |a Depine, R.A., Lakhtakia, A., (2005) New J. Phys., 7, p. 158 | ||
504 | |a Smith, D.R., Schurig, D., (2003) Phys. Rev. Lett., 90, p. 077405 | ||
504 | |a Ramakrishna, S.A., (2005) Rep. Progr. Phys., 68, p. 449 | ||
504 | |a Lakhtakia, A., Sherwin, J.A., (2003) Int. J. Infrared Millim. Waves, 24, p. 19 | ||
504 | |a Chen, H.C., (1983) Theory of Electromagnetic Waves: A Coordinate-free Approach, , McGraw-Hill New York, NY, USA | ||
504 | |a Depine, R.A., Lakhtakia, A., (2004) Opt. Commun., 233, p. 277 | ||
504 | |a Depine, R.A., Lakhtakia, A., (2004) Phys. Rev. e, 69, p. 057602 | ||
504 | |a Depine, R.A., Lakhtakia, A., (2005) Optik, 116, p. 31 | ||
504 | |a Depine, R.A., Lakhtakia, A., Smith, D.R., (2005) Phys. Lett. A, 337, p. 155 | ||
504 | |a Chandezon, J., Dupuis, M., Cornet, G., Maystre, D., (1982) J. Opt. Soc. Am., 72, p. 839 | ||
504 | |a Inchaussandague, M.E., Depine, R.A., (1996) Phys. Rev. e, 54, p. 2899 | ||
504 | |a Inchaussandague, M.E., Depine, R.A., (1997) J. Mod. Opt., 44, p. 1 | ||
504 | |a Li, L., (1999) J. Opt. Soc. Am. A, 16, p. 2521 | ||
504 | |a Li, L., Chandezon, J., Granet, G., Plumey, J.P., (1999) Appl. Opt., 38, p. 304 | ||
504 | |a Taflove, A., Hagness, S., (2005) Computational Electrodynamics: The Finite-difference Time-domain Method, , third ed. Artech House Boston, MA, USA | ||
506 | |2 openaire |e Política editorial | ||
520 | 3 | |a The differential method (also called the C method) is applied to the diffraction of linearly polarized plane waves at a periodically corrugated boundary between vacuum and a linear, homogeneous, uniaxial, dielectric-magnetic medium characterized by hyperbolic dispersion equations. Numerical results for sinusoidal gratings are presented and compared with those obtained by means of the Rayleigh method, showing that both the differential method and the Rayleigh method can fail to give adequate results for gratings supporting an infinite number of refracted Floquet harmonics. © 2005 Elsevier B.V. All rights reserved. |l eng | |
536 | |a Detalles de la financiación: 1201/OC-AR-PICT14099 | ||
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. and M.E.I. acknowledge financial support from Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET), Agencia Nacional de Promoción Científica y Tecnológica (ANPCYT-BID 1201/OC-AR-PICT14099) and Universidad de Buenos Aires. A.L. is grateful for financial support from the Penn State CIRTL Project funded by the US National Science Foundation. | ||
593 | |a Grupo de Electromagnetismo Aplicado, Departamento de Física, Pabellón I, 1428 Buenos Aires, Argentina | ||
593 | |a Consejo Nacional de Investigaciones Científicas y Técnicas, Rivadavia 1917, Buenos Aires, Argentina | ||
593 | |a Computational and Theoretical Materials Sciences Group, Department of Engineering Science and Mechanics, Pennsylvania State University, University Park, PA 16802-6812, United States | ||
593 | |a Department of Physics, Imperial College, London SW7 2BZ, United Kingdom | ||
690 | 1 | 0 | |a ANISOTROPY |
690 | 1 | 0 | |a DIFFRACTION |
690 | 1 | 0 | |a ELLIPTIC DISPERSION EQUATION |
690 | 1 | 0 | |a GRATING |
690 | 1 | 0 | |a HYPERBOLIC DISPERSION EQUATION |
690 | 1 | 0 | |a NEGATIVE REFRACTION |
690 | 1 | 0 | |a ANISOTROPY |
690 | 1 | 0 | |a DIFFRACTION GRATINGS |
690 | 1 | 0 | |a DISPERSION (WAVES) |
690 | 1 | 0 | |a HARMONIC ANALYSIS |
690 | 1 | 0 | |a LIGHT POLARIZATION |
690 | 1 | 0 | |a RAYLEIGH FADING |
690 | 1 | 0 | |a ELLIPTIC DISPERSION EQUATION |
690 | 1 | 0 | |a GRATING |
690 | 1 | 0 | |a HYPERBOLIC DISPERSION EQUATION |
690 | 1 | 0 | |a NEGATIVE REFRACTION |
690 | 1 | 0 | |a LIGHT REFRACTION |
700 | 1 | |a Inchaussandague, M.E. | |
700 | 1 | |a Lakhtakia, A. | |
773 | 0 | |d 2006 |g v. 258 |h pp. 90-96 |k n. 2 |p Opt Commun |x 00304018 |w (AR-BaUEN)CENRE-276 |t Optics Communications | |
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963 | |a VARI |