2017
DOI: 10.1364/josab.34.002310
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Goos–Hänchen shifts in an epsilon-near-zero slab

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Cited by 32 publications
(7 citation statements)
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“…The asymmetry geometric parameter M1 and M2 determine the value of the GH shift, i.e., resonance will become stronger and result in a larger GH shift for specific values of the asymmetric parameter. Here, for the stationary phase method, the lateral GH shift for the reflected and transmitted beams can be calculate by using the expression [41][42][43]…”
Section: Simulation Resultsmentioning
confidence: 99%
“…The asymmetry geometric parameter M1 and M2 determine the value of the GH shift, i.e., resonance will become stronger and result in a larger GH shift for specific values of the asymmetric parameter. Here, for the stationary phase method, the lateral GH shift for the reflected and transmitted beams can be calculate by using the expression [41][42][43]…”
Section: Simulation Resultsmentioning
confidence: 99%
“…The asymmetry geometric parameter M 1 and M 2 determine the value of the GH shift, i.e., resonance will become stronger and result in a larger GH shift for specific values of the asymmetric parameter. Here, for the stationary phase method, the lateral GH shift for the reflected and transmitted beams can be calculate by using the expression [22][23][24][25],…”
Section: Simulation Resultsmentioning
confidence: 99%
“…Since the shift at a single dielectric surface is quite small, i.e., usually subwavelength scale, much attention has been devoted to enhancing this effect by applying different materials and structures. Up to now, the enhancement has been illustrated using gradient metasurfaces [8], epsilon-near-zero slabs [9], weakly absorbing slabs [10], subwavelength gratings [11], graphene [12][13][14], a coherent medium [15], and a cavity optomechanical system [16].…”
Section: Introductionmentioning
confidence: 99%