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Hybrid states of Tamm plasmons and exciton-polaritons

Hybrid states of Tamm plasmons and exciton-polaritons. M Kaliteevski, S Brand, R A Abram , I Iorsh, A V Kavokin, T C H Liew and I A Shelykh. Plan. Tamm plasmons Coupling Tamm plasmons and exciton-polaritons Controlling exciton-polaritons. Surface plasmons. n imaginary. metal.

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Hybrid states of Tamm plasmons and exciton-polaritons

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  1. Hybrid states of Tamm plasmons and exciton-polaritons M Kaliteevski, S Brand, R A Abram, I Iorsh, A V Kavokin, T C H Liew and I A Shelykh

  2. Plan • Tamm plasmons • Coupling Tamm plasmons • and exciton-polaritons • Controlling exciton-polaritons

  3. Surface plasmons n imaginary metal imaginary imaginary vacuum Cannot be excited directly and only with E in plane of incidence (TM)

  4. Surface plasmon dispersion

  5. Tamm plasmons n imaginary metal imaginary imaginary Bragg reflector even with Can be excited at normal and oblique incidence (TE and TM)

  6. if high index layer comes first

  7. Field profile for Tamm plasmons

  8. Field intensity profile for cavity photons

  9. Resonant coupling of Tamm plasmons and exciton-polaritons

  10. Hybrid modes Three oscillator model Lowest hybrid mode is lower in energy than exciton-polariton by

  11. Real part of energy of the hybrid modes versus width of the semiconductor layer adjacent to the gold Real part of energy of the hybrid modes versus thickness of the gold layer. Vertical bars give the imaginary parts of energy

  12. In-plane dispersion curves of hybrid modes for 50 nm film of gold: solid TE, dashed TM

  13. Using surface metallization for lateral spatial control of exciton-polaritons Illuminate at a photon energy just above the lowest mode - excitations only created where there is metal

  14. Using the Stark effect and polariton bistability Pump detuning D1< D0 < D2 Reduce detuning in one segment by Stark effect – local state goes from lower red to green Diffusion into adjacent segment – local state goes from green to upper red

  15. Conclusions Technologically straightforward process of surface metallization makes it possible to have Tamm plasmons in planar microcavity structures Strong coupling of Tamm plasmons and exciton-polaritons is possible Effect can be used to provide spatial control of exciton-polaritons

  16. Acknowledgements Valuable discussions with T. Ostatnický EU FP7 funding through the POLALAS (230811) and Clermont4 (235114) projects NCCR Quantum Photonics, Swiss National Science Foundation Center of Excellence in Polaritonics, funded by RANNIS

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