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Nonlinear Wood anomalies in the reflectivity of layered superconductors
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10.1063/1.3331418
/content/aip/journal/ltp/36/3/10.1063/1.3331418
http://aip.metastore.ingenta.com/content/aip/journal/ltp/36/3/10.1063/1.3331418
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Geometry for the resonance excitations of NWGMs in a layered superconductor slab of thickness sandwiched between two dielectric prisms. The latter are separated from the layered superconductor slab by two vacuum gaps of thickness . An electromagnetic wave with angle o fincidence can excite SJPWs that satisfy the following resonance condition: . Here and are the wave-vectors of the incident and reflected waves associated with the magnetic field amplitudes and . The resonance excitation of SJPWs by the incident wave produces a strong suppression of the reflected wave. This method for producing surface waves is known as the “attenuated-total-reflection” method.

Image of FIG. 2.
FIG. 2.

The dependence of the reflectivity on the incidence angle for the two different vacuum gap widths: (dashed curve) and (solid curve). Thus the minimum value of the reflectivity for the second case equals to zero. The normalized incident wave amplitude is . Other parameters are: , , , , , , .

Image of FIG. 3.
FIG. 3.

The dependence of the reflectivity on the magnetic field amplitudes for the incidence angle . The other parameters are the same as in Fig. 2.

Image of FIG. 4.
FIG. 4.

The magnetic field distribution for the non-resonant case, , the vacuum gap widths . Other parameters are the same as in Fig. 3.

Image of FIG. 5.
FIG. 5.

The magnetic field distribution for the resonant case, . Other parameters are the same as in Fig. 4.

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/content/aip/journal/ltp/36/3/10.1063/1.3331418
2010-04-07
2014-04-24
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Nonlinear Wood anomalies in the reflectivity of layered superconductors
http://aip.metastore.ingenta.com/content/aip/journal/ltp/36/3/10.1063/1.3331418
10.1063/1.3331418
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