Unidirectional Reflectionless Propagation in Plasmonic Waveguide System Based on Phase Coupling Between Two Stub Resonators

A scheme on unidirectional reflectionless propagation is theoretically investigated in a plasmonic waveguide system which consists of two metal–insulator–metal (MIM) stub resonators side coupled to an MIM plasmonic waveguide. By appropriately tuning the phase difference between two stub resonators, unidirectional reflectionless propagation at exceptional point, phase transition, and coherent perfect absorber are realized. Moreover, in both directions, reflectivity for one side is close to 0 and for the other side approximates to 0.8.

[1]  Shanhui Fan,et al.  Broadband sharp 90-degree bends and T-splitters in plasmonic coaxial waveguides. , 2013, Nano letters.

[2]  S. Feng Loss-induced super scattering and gain-induced absorption. , 2016, Optics express.

[3]  Georgios Veronis,et al.  Unidirectional reflectionless propagation in plasmonic waveguide-cavity systems at exceptional points. , 2015, Optics express.

[4]  Hong Chen,et al.  Experimental demonstration of a coherent perfect absorber with PT phase transition. , 2014, Physical review letters.

[5]  Ru Zhang,et al.  Multiple plasmon-induced transparencies in coupled-resonator systems. , 2012, Optics letters.

[6]  Ekmel Ozbay,et al.  Two-dimensional complex parity-time-symmetric photonic structures , 2015 .

[7]  Jiaguang Han,et al.  Manifestation of PT symmetry breaking in polarization space with terahertz metasurfaces. , 2014, Physical review letters.

[8]  Ying Qiao Zhang,et al.  Polarization-independent electromagnetically induced transparency-like effects in stacked metamaterials based on Fabry–Pérot resonance , 2013 .

[9]  R. Fleury,et al.  Unidirectional Cloaking Based on Metasurfaces with Balanced Loss and Gain , 2015 .

[10]  Yadong Xu,et al.  Zero index metamaterials with PT symmetry in a waveguide system. , 2016, Optics express.

[11]  Georgios Veronis,et al.  Broadband near total light absorption in non-PT-symmetric waveguide-cavity systems. , 2016, Optics express.

[12]  Georgios Veronis,et al.  Subwavelength slow-light waveguides based on a plasmonic analogue of electromagnetically induced transparency , 2011 .

[13]  Jennifer A. Dionne,et al.  A parity-time symmetric coherent plasmonic absorber-amplifier , 2015 .

[14]  M. Segev,et al.  Observation of parity–time symmetry in optics , 2010 .

[15]  C. Bender,et al.  Real Spectra in Non-Hermitian Hamiltonians Having PT Symmetry , 1997, physics/9712001.

[16]  Vilson R. Almeida,et al.  Experimental demonstration of a unidirectional reflectionless parity-time metamaterial at optical frequencies. , 2013, Nature materials.

[17]  Pei Wang,et al.  Unidirectional reflectionless phenomenon in periodic ternary layered material. , 2016, Optics express.

[18]  Sunkyu Yu,et al.  Control of Fano asymmetry in plasmon induced transparency and its application to plasmonic waveguide modulator. , 2012, Optics express.

[19]  D. Pile,et al.  Two-dimensionally localized modes of a nanoscale gap plasmon waveguide , 2005 .

[20]  Yun Shen,et al.  Unidirectional invisibility in a two-layer non-PT-symmetric slab. , 2014, Optics express.

[21]  Zhanghua Han,et al.  Plasmon-induced transparency with detuned ultracompact Fabry-Perot resonators in integrated plasmonic devices. , 2011, Optics express.

[22]  R. Morandotti,et al.  Observation of PT-symmetry breaking in complex optical potentials. , 2009, Physical review letters.

[23]  Xueming Liu,et al.  Induced transparency in nanoscale plasmonic resonator systems. , 2011, Optics letters.

[24]  Yeshaiahu Fainman,et al.  Nonreciprocal Light Propagation in a Silicon Photonic Circuit , 2011, Science.

[25]  R. J. Bell,et al.  Optical properties of the metals Al, Co, Cu, Au, Fe, Pb, Ni, Pd, Pt, Ag, Ti, and W in the infrared and far infrared. , 1983, Applied optics.

[26]  J. Zheng,et al.  Type-II perfect absorption and amplification modes with controllable bandwidth in combined PT-symmetric and conventional Bragg-grating structures , 2014 .

[27]  Ye-Long Xu,et al.  Unidirectional Transmission Based on a Passive PT Symmetric Grating With a Nonlinear Silicon Distributed Bragg Reflector Cavity , 2014, IEEE Photonics Journal.

[28]  Jing Zhang,et al.  Optomechanically-induced transparency in parity-time-symmetric microresonators , 2014, Scientific Reports.

[29]  S. Xiao,et al.  The combination of directional outputs and single-mode operation in circular microdisk with broken PT symmetry. , 2015, Optics express.

[30]  Jennifer A. Dionne,et al.  Parity-time-symmetric plasmonic metamaterials , 2013, 1306.0059.

[31]  Jensen Li,et al.  Effective Spontaneous PT-symmetry Breaking in Hybridized Metamaterials , 2012, 1210.2027.

[32]  Shiyue Hua,et al.  Parity–time symmetry and variable optical isolation in active–passive-coupled microresonators , 2014, Nature Photonics.

[33]  Hui Cao,et al.  Unidirectional invisibility induced by PT-symmetric periodic structures. , 2011, Physical review letters.

[34]  Xueming Liu,et al.  Plasmonic nanosensor based on Fano resonance in waveguide-coupled resonators. , 2012, Optics letters.

[35]  Sailing He,et al.  Parity-Time Symmetry Breaking in Coupled Nanobeam Cavities , 2015, Scientific Reports.

[36]  D. Christodoulides,et al.  Parity-time–symmetric microring lasers , 2014, Science.

[37]  Yuan Wang,et al.  Demonstration of a large-scale optical exceptional point structure. , 2014, Optics express.

[38]  Y. Wang,et al.  Single-mode laser by parity-time symmetry breaking , 2014, Science.

[39]  Shanhui Fan,et al.  Parity–time-symmetric whispering-gallery microcavities , 2013, Nature Physics.

[40]  Mohammad-Ali Miri,et al.  Large area single-mode parity-time-symmetric laser amplifiers. , 2012, Optics letters.

[41]  Toshihiro Okamoto,et al.  Characteristics of gap plasmon waveguide with stub structures. , 2008, Optics express.

[42]  Carl M. Bender,et al.  Making sense of non-Hermitian Hamiltonians , 2007, hep-th/0703096.