Near‐Field Inductive Coupling Induced Polarization Control in Metasurfaces

Arbitrary manipulation of polarization of light has been an important research area that has applications in holography, vector beam generation, beam splitting, and design of wave plates. In this work, we investigate the near-field inductive coupling induced cross-polarized radiation in metasurfaces and its dominant role in polarization control. The inductive coupling in the chosen meta-molecular design depends on the mutual orientation of the meta-atoms that could tailor the coupling channel and thus the cross-polarized radiation is passively switched between “on” and “off” states leading to an effective control of the output polarization state of light. The non-intuitive tuning behavior of the inductively excited mode is interpreted through a circuit model where the exact location of the effective inductor in the meta-molecule dominates the coupling behavior. The switch on/off state of the coupling channel provides a new perspective of near-field coupling based passive and active control of polarization devices in applications such as holograms and encoded metamaterials.

[1]  Weili Zhang,et al.  Experimental demonstration of ultrasensitive sensing with terahertz metamaterial absorbers: A comparison with the metasurfaces , 2015 .

[2]  Jianguo Tian,et al.  Realization of broadband cross-polarization conversion in transmission mode in the terahertz region using a single-layer metasurface. , 2015, Optics letters.

[3]  D. Grischkowsky,et al.  Far-infrared time-domain spectroscopy with terahertz beams of dielectrics and semiconductors , 1990 .

[4]  Guoxing Zheng,et al.  Metasurface holograms reaching 80% efficiency. , 2015, Nature nanotechnology.

[5]  Ewold Verhagen,et al.  Electric and magnetic dipole coupling in near-infrared split-ring metamaterial arrays. , 2009, Physical review letters.

[6]  Jianxiong Li,et al.  Optical Polarization Encoding Using Graphene‐Loaded Plasmonic Metasurfaces , 2016 .

[7]  David R. Smith,et al.  Metamaterials and Negative Refractive Index , 2004, Science.

[8]  Jianguo Tian,et al.  Mid-infrared tunable optical polarization converter composed of asymmetric graphene nanocrosses. , 2013, Optics letters.

[9]  Andrew G. Glen,et al.  APPL , 2001 .

[10]  Y. Wang,et al.  Plasmon-induced transparency in metamaterials. , 2008, Physical review letters.

[11]  J. Pendry A Chiral Route to Negative Refraction , 2004, Science.

[12]  A. Arbabi,et al.  Dielectric metasurfaces for complete control of phase and polarization with subwavelength spatial resolution and high transmission. , 2014, Nature nanotechnology.

[13]  J. Bonache,et al.  Equivalent-circuit models for split-ring resonators and complementary split-ring resonators coupled to planar transmission lines , 2005, IEEE Transactions on Microwave Theory and Techniques.

[14]  C. Soukoulis,et al.  Low-loss metamaterials based on classical electromagnetically induced transparency. , 2008, Physical review letters.

[15]  Zach DeVito,et al.  Opt , 2017 .

[16]  Guoxing Zheng,et al.  Helicity multiplexed broadband metasurface holograms , 2015, Nature Communications.

[17]  Jianguo Tian,et al.  Dynamically tunable broadband mid-infrared cross polarization converter based on graphene metamaterial , 2013 .

[18]  Wei Cao,et al.  Equivalent circuit analysis of terahertz metamaterial filters , 2011 .

[19]  Weili Zhang,et al.  A Tunable Dispersion‐Free Terahertz Metadevice with Pancharatnam–Berry‐Phase‐Enabled Modulation and Polarization Control , 2015, Advanced materials.

[20]  W. Pan,et al.  Electromagnetically induced transparency (EIT)-like transmission in side-coupled complementary split-ring resonators. , 2012, Optics express.

[21]  N. Yu,et al.  Light Propagation with Phase Discontinuities: Generalized Laws of Reflection and Refraction , 2011, Science.

[22]  Abul K. Azad,et al.  Near Field Coupling in Passive and Active Terahertz Metamaterial Devices , 2013, IEEE Transactions on Terahertz Science and Technology.

[23]  Harald Giessen,et al.  Magnetoinductive and Electroinductive Coupling in Plasmonic Metamaterial Molecules , 2008 .

[24]  F. Lederer,et al.  Coupling between a dark and a bright eigenmode in a terahertz metamaterial , 2009, 0901.0365.

[25]  Harald Giessen,et al.  Coupling effects in optical metamaterials. , 2010, Angewandte Chemie.

[26]  Wenqi Zhu,et al.  Efficient polarization beam splitter pixels based on a dielectric metasurface , 2015 .

[27]  Masayoshi Tonouchi,et al.  Plasmon-induced transparency in metamaterials: Active near field coupling between bright superconducting and dark metallic mode resonators , 2013 .

[28]  Ranjan Singh,et al.  Inter and intra-metamolecular interaction enabled broadband high-efficiency polarization control in metasurfaces , 2016 .

[29]  Willie J Padilla,et al.  Perfect metamaterial absorber. , 2008, Physical review letters.

[30]  Harald Giessen,et al.  Three-dimensional optical metamaterials as model systems for longitudinal and transverse magnetic coupling. , 2008, Optics express.

[31]  Willie J Padilla,et al.  Dynamical electric and magnetic metamaterial response at terahertz frequencies , 2006, 2006 Conference on Lasers and Electro-Optics and 2006 Quantum Electronics and Laser Science Conference.

[32]  Hu Tao,et al.  Reconfigurable terahertz metamaterials. , 2009, Physical review letters.

[33]  Willie J Padilla,et al.  Terahertz Magnetic Response from Artificial Materials , 2004, Science.

[34]  Weili Zhang,et al.  Polarization Control in Terahertz Metasurfaces with the Lowest Order Rotational Symmetry , 2015 .

[35]  Qiaofeng Tan,et al.  Three-dimensional optical holography using a plasmonic metasurface , 2013, Nature Communications.

[36]  Y. Wang,et al.  An ultrathin invisibility skin cloak for visible light , 2015, Science.

[37]  Zhaocheng Liu,et al.  Emergent Functionality and Controllability in Few‐Layer Metasurfaces , 2015, Advanced materials.

[38]  F. Medina,et al.  Comparative analysis of edge- and broadside- coupled split ring resonators for metamaterial design - theory and experiments , 2003 .

[39]  M. Wegener,et al.  Twisted split-ring-resonator photonic metamaterial with huge optical activity. , 2010, Optics letters.

[40]  O. Martin,et al.  Coupling strength can control the polarization twist of a plasmonic antenna. , 2013, Nano letters.

[41]  D. R. Chowdhury,et al.  Probing the transition from an uncoupled to a strong near-field coupled regime between bright and dark mode resonators in metasurfaces , 2014 .