Goos-Hänchen effect of an extraordinary refracted beam

As known, when there is total reflection on an isotropic or anisotropic interface, the reflected ray undergoes a displacement on the interface that has been studied by a great number of authors. However, if an isotropic-uniaxial interface is considered, the condition of total reflection for one of t...

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Autor principal: Pérez, Liliana Inés
Otros Autores: Simon, María Catalina
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2006
Acceso en línea:Registro en Scopus
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Registro en la Biblioteca Digital
Aporte de:Registro referencial: Solicitar el recurso aquí
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100 1 |a Pérez, Liliana Inés 
245 1 0 |a Goos-Hänchen effect of an extraordinary refracted beam 
260 |c 2006 
270 1 0 |m Perez, L.I.; Consejo Nacional de Investigaciones Científicas y Técnicas, Buenos Aires, Argentina; email: lperez@df.uba.ar 
504 |a Fleck, J.A., Feit Jr., M.D., (1983) J. Opt. Soc. Am., 73, p. 920 
504 |a Barabás, M., Szarvas, G., (1995) Appl. Opt., 34, p. 11 
504 |a Perez, L.I., Garea, M.T., (2000) Optik, 111, p. 297 
504 |a Ciattoni, A., Crosignani, B., Di Porto, P., (2001) J. Opt. Soc. Am. A, 18, p. 1656 
504 |a Tamir, T., (1986) J. Opt. Soc. Am., 3, p. 558 
504 |a Nasalski, W., (1996) J. Opt. Soc. Am. A, 13, p. 172 
504 |a Perez, L.I., Ciocci, F., (1998) J. Mod. Opt., 45, p. 2487 
504 |a Perez, L.I., (2000) J. Mod. Opt., 47, p. 1645 
504 |a Perez, L.I., (2002) J. Opt. A: Pure Appl. Opt., 4, p. 640 
504 |a Simon, M.C., Perez, L.I., (2005) J. Mod. Opt., 52, p. 529 
504 |a Perez, L.I., Simon, M.C., Lasers and their applications (2004) SPIE, 5622, p. 1370. , 5th Iberoamerican Meeting on Optics and 8th Latin American Meeting on Optics 
504 |a Perez, L.I., Vanney, C.E., (2005) J. Mod. Opt., 52, p. 1981 
506 |2 openaire  |e Política editorial 
520 3 |a As known, when there is total reflection on an isotropic or anisotropic interface, the reflected ray undergoes a displacement on the interface that has been studied by a great number of authors. However, if an isotropic-uniaxial interface is considered, the condition of total reflection for one of the refracted rays can be fulfilled whereas the other subsists as a propagating wave. This leads to the existence of a complex displacement of the propagating refracted beam maximum that can never take place in linear isotropic interfaces. We analyse this displacement up to second order and its relationship with the phase shifts which the waves that synthesize the extraordinary propagating beam suffer under conditions of ordinary total reflection. We compare these first order non-geometric effects with those which an ordinary transmitted beam undergoes in conditions of extraordinary total reflection.  |l eng 
593 |a Consejo Nacional de Investigaciones Científicas y Técnicas, Buenos Aires, Argentina 
593 |a Facultad de Ciencias Exactas y Naturales, Departamento de Física, Universidad de Buenos Aires, Argentina 
593 |a Facultad de Ingeniería, Departamento de Física, Grupo Óptica de Interfaces, Argentina 
690 1 0 |a ANISOTROPIC INTERFACE 
690 1 0 |a ISOTROPIC-UNIAXIAL INTERFACE 
690 1 0 |a ANISOTROPY 
690 1 0 |a INTERFACES (MATERIALS) 
690 1 0 |a LIGHT PROPAGATION 
690 1 0 |a LIGHT REFRACTION 
690 1 0 |a PHASE SHIFT 
690 1 0 |a LASER BEAMS 
700 1 |a Simon, María Catalina 
773 0 |d 2006  |g v. 53  |h pp. 1011-1021  |k n. 7  |p J. Mod. Opt.  |x 09500340  |w (AR-BaUEN)CENRE-328  |t Journal of Modern Optics 
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856 4 0 |u https://doi.org/10.1080/09500340500443219  |y DOI 
856 4 0 |u https://hdl.handle.net/20.500.12110/paper_09500340_v53_n7_p1011_Perez  |y Handle 
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