Longitudinal Shift of a Microwave Beam at Total Internal Reflection

Large and negative Goos–Hänchen shift with magneto-controllability based on a ferrofluid

“…The Goos-Hänchen (GH) effect, which refers to the lateral shift from the path theoretically expected from geometrical optics when a light beam is totally reflected at the interface between two different media, was discovered by Goos and Hänchen [1] and theoretically explained by Artmann in the late 1940s [2]. Later on, the GH effect was further studied theoretically [3][4][5][6][7][8] and experimentally [9][10][11]. It has been considered in many different circumstances, such as multilayered structures [12], absorptive media [13], nonlinearities [14], chiral media [15], and photonic crystals [16].…”

Large and negative Goos–Hänchen shift with magneto-controllability based on a ferrofluid

“…The Goos-Hänchen (GH) effect, which refers to the lateral shift from the path theoretically expected from geometrical optics when a light beam is totally reflected at the interface between two different media, was discovered by Goos and Hänchen [1] and theoretically explained by Artmann in the late 1940s [2]. Later on, the GH effect was further studied theoretically [3][4][5][6][7][8] and experimentally [9][10][11]. It has been considered in many different circumstances, such as multilayered structures [12], absorptive media [13], nonlinearities [14], chiral media [15], and photonic crystals [16].…”

Large Goos-Hänchen shifts from an asymmetric configuration with single-negative materials due to surface polariton resonance

“…It has since then been further studied theoretically [12][13], and experimentally [14][15]. GH effect occurs due to the interaction of the beam with the interface [16].…”

Large and negative Goos–Hänchen shift with magneto-controllability based on a ferrofluid

“…The Goos-Hänchen (GH) effect, which refers to the lateral shift from the path theoretically expected from geometrical optics when a light beam is totally reflected at the interface between two different media, was discovered by Goos and Hänchen [1] and theoretically explained by Artmann in the late 1940s [2]. Later on, the GH effect was further studied theoretically [3][4][5][6][7][8] and experimentally [9][10][11]. It has been considered in many different circumstances, such as multilayered structures [12], absorptive media [13], nonlinearities [14], chiral media [15], and photonic crystals [16].…”

Large Goos-Hänchen shifts from an asymmetric configuration with single-negative materials due to surface polariton resonance

“…It has since then been further studied theoretically [12][13], and experimentally [14][15]. GH effect occurs due to the interaction of the beam with the interface [16].…”

Large and negative Goos–Hänchen shift with magneto-controllability based on a ferrofluid

“…The Goos-Hänchen (GH) effect, which refers to the lateral shift from the path theoretically expected from geometrical optics when a light beam is totally reflected at the interface between two different media, was discovered by Goos and Hänchen [1] and theoretically explained by Artmann in the late 1940s [2]. Later on, the GH effect was further studied theoretically [3][4][5][6][7][8] and experimentally [9][10][11]. It has been considered in many different circumstances, such as multilayered structures [12], absorptive media [13], nonlinearities [14], chiral media [15], and photonic crystals [16].…”

Large Goos-Hänchen shifts from an asymmetric configuration with single-negative materials due to surface polariton resonance

“…It has since then been further studied theoretically [12][13], and experimentally [14][15]. GH effect occurs due to the interaction of the beam with the interface [16].…”