Large tunable lateral shift in prism coupling system containing a superconducting slab
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[1] A. Mir,et al. Graphene Sensor Based on Surface Plasmon Resonance for Optical Scanning , 2019, IEEE Photonics Technology Letters.
[2] A. Farmani. Three-dimensional FDTD analysis of a nanostructured plasmonic sensor in the near-infrared range , 2019, Journal of the Optical Society of America B.
[3] Jing Zhang,et al. Large Tunable Lateral Shift from Guided Wave Surface Plasmon Resonance , 2019, Plasmonics.
[4] S. F. Shaukat,et al. Nanoscale, tunable, and highly sensitive biosensor utilizing hyperbolic metamaterials in the near-infrared range. , 2018, Applied optics.
[5] A. Mir,et al. Broadly tunable and bidirectional terahertz graphene plasmonic switch based on enhanced Goos-Hänchen effect , 2018, Applied Surface Science.
[6] Wenyi Ren,et al. Large tunable negative lateral shift from graphene-based hyperbolic metamaterials backed by a dielectric , 2018, Superlattices and Microstructures.
[7] Yuanjiang Xiang,et al. Tunable enhanced Goos–Hänchen shift of light beam reflected from graphene-based hyperbolic metamaterials , 2018 .
[8] Ali Farmani,et al. Design of a High Extinction Ratio Tunable Graphene on White Graphene Polarizer , 2018, IEEE Photonics Technology Letters.
[9] M. Sheikhi,et al. Tunable resonant Goos–Hänchen and Imbert–Fedorov shifts in total reflection of terahertz beams from graphene plasmonic metasurfaces , 2017 .
[10] M. Sheikhi,et al. Analytical modeling of highly tunable giant lateral shift in total reflection of light beams from a graphene containing structure , 2017 .
[11] Ziauddin,et al. Control of Goos–Hänchen shift via input probe field intensity , 2016 .
[12] Y. P. Lee,et al. Goos-Hanchen shift at the reflection of light from the complex structures composed of superconducting and dielectric layers , 2015, 1903.01938.
[13] M. Dressel,et al. Piston pressure cell for low-temperature infrared investigations. , 2015, The Review of scientific instruments.
[14] Rong Chen,et al. Giant and tunable Goos–Hanchen shifts for attenuated total reflection structure containing graphene , 2014 .
[15] M. Aspelmeyer,et al. Silicon optomechanical crystal resonator at millikelvin temperatures , 2014 .
[16] Y. P. Lee,et al. Effect of lateral shift of the light transmitted through a one-dimensional superconducting photonic crystal , 2013 .
[17] S. Wen,et al. Electrically controlled Goos-Hänchen shift of a light beam reflected from the metal-insulator-semiconductor structure. , 2013, Optics express.
[18] X. Dai,et al. Large and negative Goos–Hänchen shift with magneto-controllability based on a ferrofluid , 2013 .
[19] Yu Song,et al. Giant Goos-Hänchen shift in graphene double-barrier structures , 2012, 1208.2395.
[20] Weijing Kong,et al. Nearly three orders of magnitude enhancement of Goos-Hanchen shift by exciting Bloch surface wave. , 2012, Optics express.
[21] G. Sui,et al. Large positive and negative lateral optical beam shift due to long-range surface plasmon resonance , 2011 .
[22] Z. Zhou,et al. Electric control of enhanced lateral shift owing to surface plasmon resonance in Kretschmann configuration with an electro-optic crystal , 2010 .
[23] Lei Gao,et al. Temperature-dependent Goos-Hänchen shift on the interface of metal/dielectric composites. , 2009, Optics express.
[24] J. P. Woerdman,et al. Observing angular deviations in the specular reflection of a light beam , 2009 .
[25] Z. Cao,et al. Electric control of spatial beam position based on the Goos–Hänchen effect , 2008 .
[26] Xi Chen,et al. Giant bistable lateral shift owing to surface-plasmon excitation in Kretschmann configuration with a Kerr nonlinear dielectric. , 2008, Optics letters.
[27] Y. Genenko,et al. The effect of a superconducting surface layer on the optical properties of a dielectric photonic composite , 2008 .
[28] J. P. Woerdman,et al. Observation of Goos-Hänchen shifts in metallic reflection. , 2007, Optics express.
[29] H. Chiang,et al. Large negative Goos-Hanchen shift at metal surfaces , 2007 .
[30] S. Wen,et al. Negative and positive Goos–Hänchen shifts of a light beam transmitted from an indefinite medium slab , 2007 .
[31] Pengfei Zhu,et al. Large positive and negative lateral optical beam shift in prism-waveguide coupling system. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.
[32] Shi-Yao Zhu,et al. Large negative Goos-Hänchen shift from a weakly absorbing dielectric slab. , 2005, Optics letters.
[33] M. Porras. Moment-method evaluation of the angular and lateral shifts of reflected light beams , 1996 .
[34] H. Sasada,et al. Measurements of transverse lateral and longitudinal angular shifts of high-azimuthal-mode Laguerre–Gaussian beams reflected at a dielectric interface near critical incidence , 2013 .
[35] Jin Au Kong,et al. Reflection Coefficients and Goos-Hanchen Shifts in Anisotropic and Bianisotropic Left-Handed Metamaterials , 2005 .
[36] K. Artmann. Berechnung der Seitenversetzung des totalreflektierten Strahles , 1948 .
[37] F. Goos,et al. Ein neuer und fundamentaler Versuch zur Totalreflexion , 1947 .