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Implementation of PT symmetric devices using plasmonics: principle and applications

H. BenistyLaboratoire Charles Fabry de l'Institut d'Optique, CNRS, Univ. Paris-Sud, Campus Polytechnique, Palaiseau, France. [email protected]Aloyse DegironInstitut d’électronique fondamentale, UMR 8622 du CNRS, Université Paris-Sud, Bât. 220, 91405 Orsay Cedex, FranceAnatole LupuInstitut d’électronique fondamentale, UMR 8622 du CNRS, Université Paris-Sud, Bât. 220, 91405 Orsay Cedex, FranceA. de LustracInstitut d’électronique fondamentale, UMR 8622 du CNRS, Université Paris-Sud, Bât. 220, 91405 Orsay Cedex, FranceSebastien ChénaisLaboratoire de Physique des Lasers, UMR 7538, Université Paris, 13/CNRS, 93430 Villetaneuse, FranceSébastien ForgetLaboratoire de Physique des Lasers, UMR 7538, Université Paris, 13/CNRS, 93430 Villetaneuse, FranceMondher BesbesLaboratoire Charles Fabry de l¿Institut d¿Optique, CNRS, Univ Paris Sud, Campus Polytechnique RD 128, 91127 Palaiseau Cedex, FranceGrégory BarbillonLaboratoire Charles Fabry de l¿Institut d¿Optique, CNRS, Univ Paris Sud, Campus Polytechnique RD 128, 91127 Palaiseau Cedex, FranceAurélien BruyantLaboratoire de Nanotechnologie et d’Instrumentation Optique, Institut Charles Delaunay, CNRS-FRE 2848, Université de Technologie de Troyes, BP 2060, 10010 Troyes, FranceSylvain BlaizeLaboratoire de Nanotechnologie et d’Instrumentation Optique, Institut Charles Delaunay, CNRS-FRE 2848, Université de Technologie de Troyes, BP 2060, 10010 Troyes, FranceGilles LérondelLaboratoire de Nanotechnologie et d’Instrumentation Optique, Institut Charles Delaunay, CNRS-FRE 2848, Université de Technologie de Troyes, BP 2060, 10010 Troyes, France
2011en
ABI

Аннотация

The so-called PT symmetric devices, which feature ε((-x)) = ε((x))* associated with parity-time symmetry, incorporate both gain and loss and can present a singular eigenvalue behaviour around a critical transition point. The scheme, typically based on co-directional coupled waveguides, is here transposed to the case of variable gain on one arm with fixed losses on the other arm. In this configuration, the scheme exploits the full potential of plasmonics by making a beneficial use of their losses to attain a critical regime that makes switching possible with much lowered gain excursions. Practical implementations are discussed based on existing attempts to elaborate coupled waveguide in plasmonics, and based also on the recently proposed hybrid plasmonics waveguide structure with a small low-index gap, the PIROW (Plasmonic Inverse-Rib Optical Waveguide).

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