journal article·2020-12

Negative Goos-Hänchen shift induced by AC biasing voltage in ITO-silica microsphere-ITO structure

Xinbing Jiao, Fengning Sun, Lumeng Li, Xiaocong Zhang, Mingxing Zhao

Optical Materials· Volume 110
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Abstract

Abstract The Goos-Hanchen (GH) shift of a linearly polarized laser beam, reflected from an indium tin oxide (ITO)-silica microsphere-ITO structure capacitor (ISISC) is studied under an AC biasing voltage. The polarization properties and energy distribution of the optical spots are studied using a polarimeter and slit beam profiler under different frequencies and amplitudes of the AC biasing voltage. It is found that a negative GH shift occurs at a low resonance frequency of 48 Hz and above a voltage of 2.0 V. The dependence of the ISISC's reflectivity on the frequency and amplitude of the AC biasing voltage is also discussed. The changes in the negative GH shift, polarization properties, and reflectivity occur through the combined actions of the electric field and the local field of the ISISC structure.
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Research context

OpenAlex topics: Quantum optics and atomic interactions · Magneto-Optical Properties and Applications · Photonic and Optical Devices

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References (37)

Show source-provided references
1. Ein neuer und fundamentaler versuch zur total reflection10.1002/andp.19474360704 ↗
2. Neumessung des Strahlversetzungseffektes bei Totalreflexion10.1002/andp.19494400312 ↗
3. Goos-Hänchen and Imbert-Fedorov beam shifts: an overview
4. Tunable and enhanced Goos-Hänchen shift via surface plasmon resonance assisted by a coherent medium10.1364/OE.384419 ↗
5. Shift vector as the geometric origin of beam shifts10.1103/PhysRevB.100.201405 ↗
6. Surface plasmon resonance enhanced Goos-Hänchen and Imbert-Fedorov shifts of Laguerre-Gaussian beams10.1016/j.optcom.2019.04.017 ↗
7. Goos-Hänchen and Imbert Fedorov shifts at gradient metasurfaces10.1364/OE.27.011902 ↗
8. Goos-Hänchen and Imbert-Fedorov effects in weyl semimetals10.1103/PhysRevA.99.023807 ↗
9. Goos-Hänchen and Imbert-Fedorov shifts for airy beams10.1364/OL.43.001411 ↗
10. Large positive and negative Goos-Hänchen shifts near the surface plasmon resonance in subwavelength grating10.1364/OE.386472 ↗
11. Observation of Goos-Hänchen of transparency of a quantum system near a plasmonic nanostructure10.1063/1.5016481 ↗
12. Optimized weak measurements of Goos-Hänchen and Imbert Fedorov shifts in partial reflection10.1364/OE.24.006041 ↗
13. Electrically controlled Goos-Hänchen shift of a light beam reflected from the metal-insulator-semiconductor10.1364/OE.21.010430 ↗
14. Temperature-dependent Goos-Hänchen shift on the interface of metal/dielectric composites10.1364/OE.17.021433 ↗
15. Magneto-optical Goos-Hänchen effect in a prism-waveguide coupling structure10.1364/OE.22.027042 ↗
16. Electrically tunable Goos-Hänchen effect with graphene in the Terahertz regime10.1002/adom.201600303 ↗
17. Giant positive and negative Goos-Hänchen shift on dielectric grating caused by guided mode resonance
18. The frequency crossover for the Goos-Hänchen shift10.1080/09500340.2013.860199 ↗
19. Controlling optical beam shifts upon reflection from a magneto-electric liquid-crystal-based system for applications to chemical vapor sensing10.1007/s00340-017-6691-1 ↗
20. Giant goos-hänchen shifts in Au-ITO-TMDCs graphene heterostructure and its potential for high performance sensor10.3390/s20041028 ↗
21. Goos–hänchen shift in single crystal silicon induced by the electro-optic effects10.1002/pssb.201900188 ↗
22. Magnetic control of Goos-Hänchen shifts in a yttrium-iron-garnet film10.1038/srep45866 ↗
23. Controlling the Goos-Hänchen shift with external electric and magnetic fields in an electro-optic/magneto-electric heterostructure10.1063/1.4951717 ↗
24. Observation of Goos-Hänchen shifts in metallic reflection10.1364/OE.15.015928 ↗
25. Giant Goos-Hänchen effect at the reflection from left-handed metamaterials10.1063/1.1615678 ↗
26. Giant and hightly reflective Goos Hänchen shift in a metal dielectric multilayer Fano structure10.1364/OE.27.028629 ↗
27. Alipour A., Farmani Ali, Mir Ali, SiO2-silver metasurface architectures for ultrasensitive and tunable plasmonic biasing, Plasmonics, DOI: 10.1007/s11468-020-01217-4.10.1007/s11468-020-01217-4 ↗
28. Guo Y., Singh N. M., Das C.M., Ouyang Q. L., Kang L. X., Li K.B., Coquet P., Yong K.T., Two-dimensional PtSe2 theoretically enhanced Goos-Hanchen shift sensitive plasmonic biosensors, Plasmonics, DOI: 10.1007/s11468-020-01204-9.10.1007/s11468-020-01204-9 ↗
29. Three-dimensional FDTD analysis of a nanostructured plasmonic sensor in the near-infrared range10.1364/JOSAB.36.000401 ↗
30. High sensitivity terahertz biosensor based on Goos-Hanchen effect in graphere
31. Broadly tunable and bidirectional terahertz graphene plasmonic switch based on enhanced Goos-Hanchen effect10.1016/j.apsusc.2018.05.092 ↗
32. Tunable resonant Goos-Hanchen and Imbert-Fedorov shifts in total reflection of terahertz beams from graphene plasmonic metasurfaces10.1364/JOSAB.34.001097 ↗
33. Magneto-optic modulation of lateral and angular shifts in spin-orbit coupled members of the graphene family10.1364/OSAC.388574 ↗
34. Electrical power generation by mechanically modulating electrical double layers10.1038/ncomms2485 ↗
35. Unified theory for goos–hänchen and imbert–fedorov effect10.1103/PhysRevA.76.013811 ↗
36. Effects of a chiral atomic medium on the manipulation of light birefringence and lateral Goos-Hänchen shifts via Kerr nonlinearity and local field effects
37. Resonance effects on total internal reflection and lateral (Goos Hanchen) beam displacement at the interface between nonlocal and local dielectric10.1103/PhysRevB.28.5877 ↗