Stimulated emission control in Photonic Crystals: Strong coupling regime in QNM approach

2006 ◽  
Author(s):  
A. Settimi ◽  
S. Severini ◽  
C. Sibilia ◽  
M. Bertolotti ◽  
A. Napoli ◽  
...  
Keyword(s):  
Photonic Crystals ◽  
Strong Coupling ◽  
Emission Control ◽  
Stimulated Emission ◽  
Strong Coupling Regime

scholarly journals Coherent control of stimulated emission inside one dimensional photonic crystals: strong coupling regime

2006 ◽  
Vol 50 (3) ◽  
pp. 379-391 ◽  
Author(s):  
A. Settimi ◽  
S. Severini ◽  
C. Sibilia ◽  
M. Bertolotti ◽  
A. Napoli ◽  
...  
Keyword(s):  
Photonic Crystals ◽  
Strong Coupling ◽  
Coherent Control ◽  
Stimulated Emission ◽  
Strong Coupling Regime ◽  
One Dimensional

scholarly journals Coherent control of stimulated emission inside one dimensional photonic crystals: strong coupling regime

2009 ◽  
Vol 69 (4) ◽  
pp. 613-614
Author(s):  
A. Settimi ◽  
S. Severini ◽  
C. Sibilia ◽  
M. Bertolotti ◽  
A. Napoli ◽  
...  
Keyword(s):  
Photonic Crystals ◽  
Strong Coupling ◽  
Coherent Control ◽  
Stimulated Emission ◽  
Strong Coupling Regime ◽  
One Dimensional

Strong Coupling: Polariton Bose Condensation

2017 ◽  
Author(s):  
Alexey V. Kavokin ◽  
Jeremy J. Baumberg ◽  
Guillaume Malpuech ◽  
Fabrice P. Laussy
Keyword(s):  
Strong Coupling ◽  
Room Temperature ◽  
Elevated Temperatures ◽  
Dissipative System ◽  
Bose Condensation ◽  
Einstein Condensation ◽  
Strong Coupling Regime ◽  
Stimulated Scattering ◽  
Exciton Polaritons ◽  
Bose Einstein

In this Chapter we address the physics of Bose-Einstein condensation and its implications to a driven-dissipative system such as the polariton laser. We discuss the dynamics of exciton-polaritons non-resonantly pumped within a microcavity in the strong coupling regime. It is shown how the stimulated scattering of exciton-polaritons leads to formation of bosonic condensates that may be stable at elevated temperatures, including room temperature.

Strong coupling: resonant effects

2017 ◽  
Author(s):  
Alexey V. Kavokin ◽  
Jeremy J. Baumberg ◽  
Guillaume Malpuech ◽  
Fabrice P. Laussy
Keyword(s):  
Strong Coupling ◽  
Experimental Studies ◽  
Strong Coupling Regime ◽  
Theoretical Studies ◽  
Stimulated Scattering ◽  
Quantum Theories ◽  
Pump Probe ◽  
Exciton Polaritons ◽  
Linear Optical Properties ◽  
Experimental And Theoretical Studies

This chapter presents experimental studies performed on planar semiconductor microcavities in the strong-coupling regime. The first section reviews linear experiments performed in the 1990s that evidence the linear optical properties of cavity exciton-polaritons. The chapter is then focused on experimental and theoretical studies of resonantly excited microcavity emission. We mainly describe experimental configuations in which stimulated scattering was observed due to formation of a dynamical condensate of polaritons. Pump-probe and cw experiments are described in addition. Dressing of the polariton dispersion and bistability of the polariton system due to inter-condensate interactions are discussed. The semiclassical and the quantum theories of these effects are presented and their results analysed. The potential for realization of devices is also discussed.

Strong-coupling regime in pillar semiconductor microcavities

1997 ◽  
Vol 22 (3) ◽  
pp. 371-374 ◽  
Author(s):  
J. Bloch ◽  
R. Planel ◽  
V. Thierry-Mieg ◽  
J.M. Gérard ◽  
D. Barrier ◽  
...  
Keyword(s):  
Strong Coupling ◽  
Strong Coupling Regime ◽  
Semiconductor Microcavities

INDICATIONS OF A ΔI=1/2 RULE IN THE STRONG COUPLING REGIME

1988 ◽  
Vol 03 (06) ◽  
pp. 1385-1412
Author(s):  
IAN G. ANGUS
Keyword(s):  
Lattice Qcd ◽  
Strong Coupling ◽  
Computer Algebra ◽  
Free Parameter ◽  
Hamiltonian Formalism ◽  
Strong Coupling Expansion ◽  
Calculation Scheme ◽  
Strong Coupling Regime ◽  
Weak Decays ◽  
The One

We will attempt to understand the ΔI=1/2 pattern of the nonleptonic weak decays of the kaons. The calculation scheme employed is the Strong Coupling Expansion of lattice QCD. Kogut-Susskind fermions are used in the Hamiltonian formalism. We will describe in detail the methods used to expedite this calculation, all of which was done by computer algebra. The final result is very encouraging. Even though an exact interpretation is clouded by the presence of irrelevant operators, and questions of lattice artifacts, a signal of the ΔI=1/2 rule appears to be observable. With an appropriate choice of the one free parameter, enhancements greater than those observed experimentally can be obtained. We also point out a number of surprising results which we turn up in the course of the calculation.

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