Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths

Dominik Floess; Jessie Y Chin; Akihito Kawatani; Daniel Dregely; Hanns-Ulrich Habermeier; Thomas Weiss; Harald Giessen

doi:10.1038/lsa.2015.57

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Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths

Original Articles

- Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths
- Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths
- LSA 2015年4卷第2期
- Affiliations：
  
  1.4th Physics Institute and Research Center SCOPE, University of Stuttgart, 70550 Stuttgart, Germany
  2.Max Planck Institute for Solid State Research, 70569 Stuttgart, Germany
- Author bio：
  
  D Floess, 4th Physics Institute and Research Center SCOPE, University of Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart, Germany Email: d.floess@pi4.uni-stuttgart.de
  H Giessen, 4th Physics Institute and Research Center SCOPE, University of Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart, Germany Email: h.giessen@pi4.uni-stuttgart.de
- Funds：
- DOI：10.1038/lsa.2015.57
  中图分类号：
- 纸质出版日期：2015-06，
  
  网络出版日期：2015-02-05，
  
  收稿日期：2014-10-16，
  
  修回日期：2015-02-03，
  
  录用日期：2015-02-04
- Accepted：
Scan QR Code
Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths[J]. LSA, 2015,4(2).

Floess, D. et al. Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths. Light: Science & Applications, 4, e284 (2015).
Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths[J]. LSA, 2015,4(2). DOI： 10.1038/lsa.2015.57.

Floess, D. et al. Tunable and switchable polarization rotation with non-reciprocal plasmonic thin films at designated wavelengths. Light: Science & Applications, 4, e284 (2015). DOI： 10.1038/lsa.2015.57.

摘要

Abstract

We experimentally demonstrate an ultra-thin plasmonic optical rotator in the visible regime that induces a polarization rotation that is continuously tunable and switchable by an external magnetic field. The rotator is a magneto-plasmonic hybrid structure consisting of a magneto-optical EuSe slab and a one-dimensional plasmonic gold grating. At low temperatures

EuSe possesses a large Verdet constant and exhibits Faraday rotation

which does not saturate over a regime of several Tesla. By combining these properties with plasmonic Faraday rotation enhancement

a large tuning range of the polarization rotation of up to 8.4° for a film thickness of 220 nm is achieved. Furthermore

through experiments and simulations

we demonstrate that the unique dispersion properties of the structure enable us to tailor the wavelengths of the tunable polarization rotation to arbitrary spectral positions within the transparency window of the magneto-optical slab. The demonstrated concept might lead to important

highly integrated

non-reciprocal

photonic devices for light modulation

optical isolation

and magnetic field optical sensing. The simple fabrication of EuSe nanostructures by physical vapor deposition opens the way for many potentially interesting magneto-plasmonic systems and three-dimensional magneto-optical metamaterials.

关键词

Keywords

active tuningFaraday rotationmagneto-opticsnon-reciprocityoptical rotator

references

Körner T, Heinrich A, Weckerle M, Roocks P, Stritzker B. Integration of magneto-optical active bismuth iron garnet on nongarnet substrates.J Appl Phys2008;103: 07B337..

Kahl S, Grishin AM. Evolution of properties of epitaxial bismuth iron garnet films with increasing thickness.J Magn Magn Mater2004;278: 244–255..

Višňovský Š, Pařízek V, Nývlt M, Kielar P, Prosser Vet al. Magneto-optical Kerr spectra of nickel.J Magn Magn Mater1993;127: 135–139..

Sepúlveda B, González-Díaz JB, García-Martín A, Lechuga LM, Armelles G. Plasmon-induced magneto-optical activity in nanosized gold disks.Phys Rev Lett2010;104: 147401..

González-Díaz JB, Sepúlveda B, García-Martín A, Armelles G. Cobalt dependence of the magneto-optical response in magnetoplasmonic nanodisks.Appl Phys Lett2010;97: 043114..

Feng HY, Luo F, Kekesi R, Granados D, Meneses-Rodríguez Det al. Magnetoplasmonic nanorings as novel architectures with tunable magneto-optical activity in wide wavelength ranges.Adv Opt Mater2014;2: 612–617..

Penfold C, Collins RT, Tufaile AP, Souche Y. Transverse magneto-optical Kerr effect: the phase change of reflected light.J Magn Magn Mater2002;242–245: 964–966..

Belotelov VI, Akimov IA, Pohl M, Kotov VA, Kasture Set al. Enhanced magneto-optical effects in magnetoplasmonic crystals.Nat Nanotechnol2011;6: 370–376..

Kreilkamp LE, Belotelov VI, Chin JY, Neutzner S, Dregely Det al. Waveguide-plasmon polaritons enhance transverse magneto-optical kerr effect.Phys Rev X2013;3: 041019..

Belotelov VI, Kreilkamp LE, Akimov IA, Kalish AN, Bykov DAet al. Plasmon-mediated magneto-optical transparency.Nat Commun2013;4: 2128..

Pavlov VV, Pisarev RV, Kirilyuk A, Rasing T. Observation of a transversal nonlinear magneto-optical effect in thin magnetic garnet films.Phys Rev Lett1997;78: 2004–2007..

Kaminski B, Lafrentz M, Pisarev RV, Yakovlev DR, Pavlov VVet al. Spin-induced optical second harmonic generation in the centrosymmetric magnetic semiconductors EuTe and EuSe.Phys Rev Lett2009;103: 057203..

Lafrentz M, Brunne D, Kaminski B, Pavlov VV, Henriques ABet al. Optical third-harmonic spectroscopy of the magnetic semiconductor EuTe.Phys Rev B2010;82: 235206..

Lafrentz M, Brunne D, Kaminski B, Pavlov VV, Pisarev RVet al. Optical third harmonic generation in the magnetic semiconductor EuSe.Phys Rev B2012;85: 035206..

Matsubara M, Schmehl A, Mannhart J, Schlom DG, Fiebig M. Giant third-order magneto-optical rotation in ferromagnetic EuO.Phys Rev B2012;86: 195127..

Davoyan AR, Engheta N. Nonreciprocal rotating power flow within plasmonic nanostructures.Phys Rev Lett2013;111: 047401..

Davoyan AR, Engheta N. Nanoscale plasmonic circulator.New J Phys2013;15: 083054..

Sun L, Jiang S, Marciante JR. All-fiber optical magnetic-field sensor based on Faraday rotation in highly terbium-doped fiber.Opt Express2010;18: 5407–5412..

Deeter MN, Rose AH, Day GW. Fast, sensitive magnetic-field sensors based on the Faraday effect in YIG.J Light Technol1990;8: 1838–1842..

Ross WE, Psaltis D, Anderson RH. Two-dimensional magneto-optic spatial light modulator for signal processing.Opt Eng1983;22: 224485..

Zhang S, Zhou JF, Park YS, Rho J, Singh Ret al. Photoinduced handedness switching in terahertz chiral metamolecules.Nat Commun2012;3: 942..

de Hoop AT. A reciprocity theorem for the electromagnetic field scattered by an obstacle.Appl Sci Res Sect B1960;8: 135–140..

Potton RJ. Reciprocity in optics.Rep Prog Phys2004;67: 717–754..

Shirasaki M, Asama K. Compact optical isolator for fibers using birefringent wedges.Appl Opt1982;21: 4296–4299..

Bi L, Hu JJ, Jiang P, Kim DH, Dionne GFet al. On-chip optical isolation in monolithically integrated non-reciprocal optical resonators.Nat Photonics2011;5: 758–762..

Fan L, Wang J, Varghese LT, Shen H, Niu Bet al. An all-silicon passive optical diode.Science2012;335: 447–450..

Ikushima I, Maeda M. Self-coupled phenomena of semiconductor lasers caused by an optical fiber.IEEE J Quantum Electron1978;14: 331–332..

Morikawa T, Mitsuhashi Y, Shimada J, Kojima Y. Return-beam-induced oscillations in self-coupled semiconductor lasers.Electron Lett1976;12: 435–436..

Petermann K. External optical feedback phenomena in semiconductor lasers.IEEE J Sel Top Quantum Electron1995;1: 480–489..

Menzel C, Helgert C, Rockstuhl C, Kley EB, Tünnermann Aet al. Asymmetric transmission of linearly polarized light at optical metamaterials.Phys Rev Lett2010;104: 253902..

Fan SH, Baets R, Petrov A, Yu ZF, Joannopoulos JDet al. Comment on "Nonreciprocal light propagation in a silicon photonic circuit".Science2012;335: 38..

Zhou Y, Dong YQ, Fan RH, Hu Q, Peng RWet al. Asymmetric transmission of terahertz waves through a graphene-loaded metal grating.Appl Phys Lett2014;105: 041114..

IntegratedPhotonics. com. Magneto-Optic LPE Garnet Faraday Rotator Crystals. Available athttp://integratedphotonics.com/products/bigfaradayrotators.htmlhttp://integratedphotonics.com/products/bigfaradayrotators.html(accessed 23 July 2014).

Thorlabs online catalog. Available athttp://www.thorlabs.dehttp://www.thorlabs.de(accessed 23 July 2014).

Liu M, Zhang X. Plasmon-boosted magneto-optics.Nat Photonics2013;7: 429–430..

Chin JY, Steinle T, Wehlus T, Dregely D, Weiss Tet al. Nonreciprocal plasmonics enables giant enhancement of thin-film Faraday rotation.Nat Commun2013;4: 1599..

Belotelov VI, Doskolovich LL, Zvezdin AK. Extraordinary magneto-optical effects and transmission through metal-dielectric plasmonic systems.Phys Rev Lett2007;98: 077401..

Gevorkian Z, Gasparian V. Plasmon-enhanced Faraday rotation in thin films.Phys Rev A2014;89: 023830..

Christ A, Tikhodeev SG, Gippius NA, Kuhl J, Giessen H. Waveguide-plasmon polaritons: strong coupling of photonic and electronic resonances in a metallic photonic crystal slab.Phys Rev Lett2003;91: 183901..

Christ A, Zentgraf T, Kuhl J, Tikhodeev SG, Gippius NAet al. Optical properties of planar metallic photonic crystal structures: experiment and theory.Phys Rev B2004;70: 125113..

Linden S, Kuhl J, Giessen H. Controlling the interaction between light and gold nanoparticles: selective suppression of extinction.Phys Rev Lett2001;86: 4688–4691..

Suits JC, Argyle BE. Paramagnetic faraday rotation of EuSe.J Appl Phys1965;36: 1251–1252..

Shen YR, Bloembergen N. Faraday rotation of rare-earth ions in CaF2. Ⅱ. Experiments.Phys Rev1964;133: A515–A520..

Schoenes J, Wachter P. High field magneto-optical study of EuSe and EuTe.Phys B+C1977;89: 155–158..

Suits JC, Argyle BE. Magnetic birefringence of EuSe.Phys Rev Lett1965;14: 687–689..

Mahan JE.Physical Vapor Deposition of Thin Films. Weinheim: Wiley-VCH; 2000.

Fan SH. Nanophotonics: magnet-controlled plasmons.Nat Photonics2010;4: 76–77..

Wehlus T, Körner T, Leitenmeier S, Heinrich A, Stritzker B. Magneto-optical garnets for integrated optoelectronic devices.Phys Status Solidi A2011;208: 252–263..

Vieu C, Carcenac F, Pépin A, Chen Y, Mejias Met al. Electron beam lithography: resolution limits and applications.Appl Surf Sci2000;164: 111–117..

Codixx ColorPol Polarizer. Prod. number VIS 052 AC3 005299, 2013.

Li LF. Fourier modal method for crossed anisotropic gratings with arbitrary permittivity and permeability tensors.J Opt A: Pure Appl Opt2003;5: 345–355..

Tikhodeev SG, Yablonskii AL, Muljarov EA, Gippius NA, Ishihara T. Quasiguided modes and optical properties of photonic crystal slabs.Phys Rev B2002;66: 045102..

Weiss T, Granet G, Gippius NA, Tikhodeev SG, Giessen H. Matched coordinates and adaptive spatial resolution in the Fourier modal method.Opt Express2009;17: 8051–8061..

Weiss T, Gippius NA, Tikhodeev SG, Granet G, Giessen H. Derivation of plasmonic resonances in the Fourier modal method with adaptive spatial resolution and matched coordinates.J Opt Soc Am A: Opt Image Sci Vis2011;28: 238–244..

Johnson PB, Christy RW. Optical constants of the noble metals.Phys Rev B1972;6: 4370–4379..

Etchegoin PG, Le Ru EC, Meyer M. An analytic model for the optical properties of gold.J Chem Phys2006;125: 164705..

Güntherodt G, Schoenes J, Wachter P. Optical constants of the Eu chalcogenides above and below the magnetic ordering temperatures.J Appl Phys1970;41: 1083–1084..

Guo HC, Nau D, Radke A, Zhang XP, Stodolka Jet al. Large-area metallic photonic crystal fabrication with interference lithography and dry etching.Appl Phys B2005;81: 271–275..

Bagheri S, Giessen H, Neubrech F. Large-area antenna-assisted SEIRA substrates by laser interference lithography.Adv Opt Mater2014;2: 1050–1056..

Wang X, Venugopal G, Zeng JW, Chen YN, Lee DHet al. Optical fiber metamagnetics.Opt Express2011;19: 19813–19821..

Lin YB, Zou Y, Mo YY, Guo JP, Lindquist RG. E-beam patterned gold nanodot arrays on optical fiber tips for localized surface plasmon resonance biochemical sensing.Sensors2010;10: 9397–9406..

Zeng X, Jradi S, Proust J, Bachelot R, Zhang ZPet al. Direct functionalization of an optical fiber by a plasmonic nanosensor.Opt Lett2011;36: 2919–2921..

Dentz DJ, Puttbach RC, Belt RF. Terbium gallium garnet for Faraday effect devices.AIP Conf Proc1974;18: 954–958..

Ahn KY, Suits JC. Preparation and properties of EuO films.IEEE Trans Magn1967;MAG-3: 453–455..

Schoenes J, Wachter P. Exchange optics in Gd-doped EuO.Phys Rev B1974;9: 3097–3105..

Shafer MW, McGuire TR. Studies of Curie-point increases in EuO.J Appl Phys1968;39: 588–590..

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