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Oscillating wave sensor based on the Goos–Hänchen effect
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10.1063/1.2883929
/content/aip/journal/apl/92/6/10.1063/1.2883929
http://aip.metastore.ingenta.com/content/aip/journal/apl/92/6/10.1063/1.2883929
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Configuration of the sensor. The parameters are as follows: , , , , , and .

Image of FIG. 2.
FIG. 2.

(solid curve) and (dashed curve) vs effective RI for the ultrahigh-order mode, simulated in stationary-phase method. The incident beam is TE polarized and in wavelength.

Image of FIG. 3.
FIG. 3.

Principle of measurement by monitoring the change of GH shift caused by the variation of RI of the guiding layer. The parameters are as follows: , for pure water (solid curve), ; for NaCl solution (dashed curve), ; waist radius is .

Image of FIG. 4.
FIG. 4.

Schematic drawing of the experimental setup.

Image of FIG. 5.
FIG. 5.

The Goos–Hänchen shifts with respect to solutions of different concentrations in the sample cell: (a) pure water, (b) NaCl solution, (c) NaCl solution, (d) NaCl solution, and (e) NaCl solution.

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/content/aip/journal/apl/92/6/10.1063/1.2883929
2008-02-15
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Oscillating wave sensor based on the Goos–Hänchen effect
http://aip.metastore.ingenta.com/content/aip/journal/apl/92/6/10.1063/1.2883929
10.1063/1.2883929
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