Critical coupling layer thickness for positive or negative Goos-Hänchen shifts near the excitation of backward surface polaritons in Otto-ATR systems

We present a theoretical analysis of the lateral displacement (Goos-Hänchen shift) of spatially limited beams reflected from attenuated total reflection (ATR) devices in the Otto configuration when backward surface plasmon polaritons are excited at the interface between a positive refractive index s...

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Autor principal: Zeller, M.A
Otros Autores: Cuevas, Mauro, Depine, Ricardo Angel
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: Institute of Physics Publishing 2015
Acceso en línea:Registro en Scopus
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100 1 |a Zeller, M.A. 
245 1 0 |a Critical coupling layer thickness for positive or negative Goos-Hänchen shifts near the excitation of backward surface polaritons in Otto-ATR systems 
260 |b Institute of Physics Publishing  |c 2015 
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504 |a Zeller, M.A., Cuevas, M., Depine, R.A., Phase and reflectivity behavior near the excitation of surface plasmon polaritons in Kretschmann-ATR systems with metamaterials (2012) Eur. Phys. J., 66, pp. 1-7 
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506 |2 openaire  |e Política editorial 
520 3 |a We present a theoretical analysis of the lateral displacement (Goos-Hänchen shift) of spatially limited beams reflected from attenuated total reflection (ATR) devices in the Otto configuration when backward surface plasmon polaritons are excited at the interface between a positive refractive index slab and a semi-infinite metamaterial with a negative refractive index. First, the stationary phase approximation and a phenomenological model based on the properties of the complex poles and zeroes of the reflection coefficient are used to demonstrate that: (i) the excitation of backward surface waves can lead to both negative and positive (and not exclusively negative) Goos-Hänchen shifts, and (ii) the sign of the shift depends on whether the value of the coupling layer thickness is higher or lower than a critical value characteristic of the ATR structure. Then, these findings are verified through rigorous calculations of the spatial structure of the reflected beam. For incident beams with a Gaussian profile, the lateral shift calculated as the first moment of the field distribution of the reflected beam agrees quite well with the predictions of approximate analysis. Near the resonant excitation of the backward surface plasmon polariton, large (negative or positive) Goos-Hänchen shifts are obtained, along with a splitting of the reflected beam. © 2015 IOP Publishing Ltd.  |l eng 
593 |a Departamento de Física, Universidad de Buenos Aires, IFIBA, Ciudad Universitaria, Pabellón I, Buenos Aires, C1428EHA, Argentina 
690 1 0 |a ATTENUATED TOTAL REFLECTION 
690 1 0 |a BACKWARD WAVES 
690 1 0 |a LATERAL SHIFT 
690 1 0 |a LIMITED BEAMS 
690 1 0 |a METAMATERIALS 
690 1 0 |a SURFACE PLASMONS 
690 1 0 |a ELECTROMAGNETIC WAVE POLARIZATION 
690 1 0 |a ELECTROMAGNETIC WAVE REFLECTION 
690 1 0 |a EXCITED STATES 
690 1 0 |a METAMATERIALS 
690 1 0 |a PARTICLE OPTICS 
690 1 0 |a PHONONS 
690 1 0 |a PHOTONS 
690 1 0 |a PLASMONS 
690 1 0 |a QUANTUM THEORY 
690 1 0 |a REFRACTIVE INDEX 
690 1 0 |a SURFACE PLASMON RESONANCE 
690 1 0 |a SURFACE WAVES 
690 1 0 |a ATTENUATED TOTAL REFLECTIONS 
690 1 0 |a BACKWARD WAVES 
690 1 0 |a LATERAL SHIFTS 
690 1 0 |a LIMITED BEAMS 
690 1 0 |a SURFACE PLASMONS 
690 1 0 |a GAUSSIAN BEAMS 
700 1 |a Cuevas, Mauro 
700 1 |a Depine, Ricardo Angel 
773 0 |d Institute of Physics Publishing, 2015  |g v. 17  |h pp. 1-8  |k n. 5  |p J. Opt.  |x 20408978  |t Journal of Optics (United Kingdom) 
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