1.The MOE Key Laboratory of Weak Light Nonlinear Photonics, School of Physics, Teda Applied Physics Institute, and the 2011 Project Collaborative Innovation Center for Biological Therapy, Nankai University, Tianjin 300071, China
2.Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
Optical activity is the rotation of the plane of linearly polarized light along the propagation direction as the light travels through optically active materials. In existing methods
the strength of the optical activity is determined by the chirality of the materials
which is difficult to control quantitatively. Here we numerically and experimentally investigated an alternative approach to realize and control the optical activity with non-chiral plasmonic metasurfaces. Through judicious design of the structural units of the metasurfaces
the right and left circular polarization components of the linearly polarized light have different phase retardations after transmitting through the metasurfaces
leading to large optical activity. Moreover
the strength of the optical activity can be easily and accurately tuned by directly adjusting the phase difference. The proposed approach based on non-chiral plasmonic metasurfaces exhibits large optical activity with a high controllable degree of freedom
which may provide more possibilities for applications in photonics.
Kuzmenko AM, Shuvaev A, Dziom V, Pimenov A, Schiebl Met al. Giant gigahertz optical activity in multiferroic ferroborate.Phys Rev B2014;89: 174407..
Park HS, Kim TT, Kim HD, Kim K, Min B. Nondispersive optical activity of meshed helical metamaterials.Nat Commun2014;5: 5435..
Barron LD.Molecular Light Scattering and Optical Activity. Cambridge: Cambridge University Press; 2004.
Ogawa N, Seki S, Tokura Y. Ultrafast optical excitation of magnetic skyrmions.Sci Rep2015;5: 9552..
Okamura Y, Kagawa F, Seki S, Kubota M, Kawasaki Met al. Microwave magnetochiral dichroism in the chiral-lattice magnet Cu2OSeO3.Phys Rev Lett2015;114: 197202..
Zheludev NI. The road ahead for metamaterials.Science2010;328: 582–583..
Liu YM, Zhang X. Metamaterials: a new frontier of science and technology.Chem Soc Rev2011;40: 2494–2507..
Zheludev NI. Obtaining optical properties on demand.Science2015;348: 973–974..
Shelby RA, Smith DR, Schultz S. Experimental verification of a negative index of refraction.Science2001;292: 77–79..
Valentine J, Zhang S, Zentgraf T, Ulin-Avila E, Genov DAet al. Three-dimensional optical metamaterial with a negative refractive index.Nature2008;455: 376–379..
Nguyen VC, Chen L, Halterman K. Total transmission and total reflection by zero index metamaterials with defects.Phys Rev Lett2010;105: 233908..
Liu N, Wen FF, Zhao Y, WangYM, Nordlander Pet al. Individual nanoantennas loaded with three-dimensional optical nanocircuits.Nano Lett2013;13: 142–147..
Cui YH, Kang L, Lan SF, Rodrigues S, Cai WS. Giant chiral optical response from a twisted-arc metamaterial.Nano Lett2014;14: 1021–1025..
Kuwata-Gonokami M, Saito N, Ino Y, Kauranen M, Jefimovs Ket al. Giant optical activity in quasi-two-dimensional planar nanostructures.Phys Rev Lett2005;95: 227401..
Bai B, Svirko Y, Turunen J, Vallius T. Optical activity in planar chiral metamaterials: theoretical study.Phys Rev A2007;76: 023811..
Yin XH, Schäferling M, Metzger B, Giessen H. Interpreting chiral nanophotonic spectra: the plasmonic Born-Kuhn model.Nano Lett2013;13: 6238–6243..
Li ZF, Mutlu M, Ozbay E. Chiral metamaterials: from optical activity and negative refractive index to asymmetric transmission.J Opt2013;15: 023001..
Kang L, Lan SF, Cui YH, Rodrigues SP, Liu YMet al. An active metamaterial platform for chiral responsive optoelectronics.Adv Mater2015;27: 4377–4383..
Yu NF, Genevet P, Kats MA, Aieta F, Tetienne JPet al. Light propagation with phase discontinuities: generalized laws of reflection and refraction.Science2011;334: 333–337..
Yu NF, Capasso F. Flat optics with designer metasurfaces.Nat Mater2014;13: 139–150..
Cheng H, Liu ZC, Chen SQ, Tian JG. Emergent functionality and controllability in few-layer metasurfaces.Adv Mater2015;27: 5410–5421..
Yin XB, Ye ZL, Rho J, Wang Y, Zhang X. Photonic spin Hall effect at metasurfaces.Science2013;339: 1405–1407..
Li T, Liu H, Wang SM, Yin XG, Wang FMet al. Manipulating optical rotation in extraordinary transmission by hybrid plasmonic excitations.Appl Phys Lett2008;93: 021110..
Cheng H, Chen SQ, Yu P, Li JX, Deng Let al. Mid-infrared tunable optical polarization converter composed of asymmetric graphene nanocrosses.Opt Lett2013;38: 1567–1569..
Grady NK, Heyes JE, Chowdhury DR, Zeng Y, Reiten MTet al. Terahertz metamaterials for linear polarization conversion and anomalous refraction.Science2013;340: 1304–1307..
Shaltout A, Liu JJ, Shalaev VM, Kildishev AV. Optically active metasurface with non-chiral plasmonic nanoantennas.Nano Lett2014;14: 4426–4431..
Jiang SC, Xiong X, Hu YS, Jiang SW, Hu YHet al. High-efficiency generation of circularly polarized light via symmetry-induced anomalous reflection.Phys Rev B2015;91: 125421..
Li JX, Chen SQ, Yang HF, Li JJ, Yu Pet al. Simultaneous control of light polarization and phase distributions using plasmonic metasurfaces.Adv Funct Mater2015;25: 704–710..
Shitrit N, Nechayev S, Kleiner V, Hasman E. Spin-dependent plasmonics based on interfering topological defects.Nano Lett2012;12: 1620–1623..
Yang YM, Wang WY, Moitra P, Kravchenko Ⅱ, Briggs DPet al. Dielectric meta-reflectarray for broadband linear polarization conversion and optical vortex generation.Nano Lett2014;14: 1394–1399..
Yu P, Chen SQ, Li JX, Cheng H, Li ZCet al. Generation of vector beams with arbitrary spatial variation of phase and linear polarization using plasmonic metasurfaces.Opt Lett2015;40: 3229–3232..
Zhao Y, Alù A. Tailoring the dispersion of plasmonic nanorods to realize broadband optical meta-wave plates.Nano Lett2013;13: 1086–1091..
Yu NF, Aieta F, Genevet P, Kats MA, Gaburro Zet al. A broadband, background-free quarter-wave plate based on plasmonic metasurfaces.Nano Lett2012;12: 6328–6333..
Zhao Y, Alù A. Manipulating light polarization with ultrathin plasmonic metasurfaces.Phys Rev B2011;84: 205428..
Li T, Wang SM, Cao JX, Liu H, Zhu SN. Cavity-involved plasmonic metamaterial for optical polarization conversion.Appl Phys Lett2010;97: 261113..
Baida FI, Boutria M, Oussaid R, Labeke DV. Enhanced-transmission metamaterials as anisotropic plates.Phys Rev B2011;84: 035107..
Wu S, Zhang Z, Zhang Y, Zhang KY, Zhou Let al. Enhanced rotation of the polarization of a light beam transmitted through a silver film with an array of perforated S-shaped holes.Phys Rev Lett2013;110: 207401..
Liu WW, Chen SQ, Li ZC, Cheng H, Yu Pet al. Realization of broadband cross-polarization conversion in transmission mode in the terahertz region using a single-layer metasurface.Opt Lett2015;40: 3185–3188..
Johnson PB, Christy RW. Optical constants of the noble metals.Phys Rev B1972;6: 4370–4379..
Born M, Wolf E.Principles of Optics. Cambridge: Cambridge University Press; 1999.
Gori F. Measuring Stokes parameters by means of a polarization grating.Opt Lett1999;24: 584–586..
Liu ZC, Chen SQ, Li JX, Cheng H, Li ZCet al. Fully interferometric controllable anomalous refraction efficiency using cross modulation with plasmonic metasurfaces.Opt Lett2014;39: 6763–6766..
Roberts A, Lin L. Plasmonic quarter-wave plate.Opt Lett2012;37: 1820–1822..
Bifunctional gap-plasmon metasurfaces for visible light: polarization-controlled unidirectional surface plasmon excitation and beam steering at normal incidence
All-optical dynamic focusing of light via coherent absorption in a plasmonic metasurface
Giant intrinsic chiro-optical activity in planar dielectric nanostructures
Beam switching and bifocal zoom lensing using active plasmonic metasurfaces
Fano-resonance-assisted metasurface for color routing
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