Teoria quantistica: Polaritone.

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Presentation transcript:

Teoria quantistica: Polaritone

Teoria quantistica: Polaritone

Sommario eccitone Stato isolato nel gap Transizione tunabile Spin intero Picco di assorbimento ben separato dal continuo e-h Stato isolato nel gap Transizione tunabile Statistica bosonica Moto libero nel piano (k//)

Sommario MC Stato isolato nel gap Transizione tunabile Statistica bosonica Moto libero nel piano (k//)

Sommario interazione classica bare photon bare exciton bare exciton bare photon

Photon state in second quantization and k space Electromagnetic Vacuum

Funzione inviluppo eccitone Eccitone 1s (prima quantizzazione) +e -e Funzione inviluppo eccitone

Elettroni e lacune in seconda quantizzazione Onda CB Onda VB Linguaggio elettroni

Linguaggio elettroni

Half-photon, half-exciton

Anticrossing k//=0

Accordo in frequenza Controllo deterministico del tuning a posteriori Cavità con gradiente

GaAs

Effetti quantistici BEC polaritoni

Anticrossing k//=0

Lower polariton states

Bose-Einstein condensation (BEC) of an ideal Bose gas1 The Bose-Einstein distribution function: In a d-dimensional system with a parabolic dispersion around k=0: In a 3D (d=3) system with a parabolic dispersion around k=0: 1 S.N. Bose, Z. Phys. 26, 178 (1924), A. Einstein, Sitzber. Kgl. Preuss. Akad. Wiss (1924).

Scattering risonante

Fononi distruggono strong coupling

Exciton scattering distrugge strong coupling

Esistenza polaritone Broadening distrugge Strong coupling Coupling regimes Broadening distrugge Strong coupling

Phase diagram of exciton-polaritons Weak coupling Weak coupling Strong coupling Solid lines show the critical concentration Nc versus temperature of the polariton KT phase transition. Dotted and dashed lines show the critical concentration Nc for quasi condensation in 100 µm and 1 meter lateral size systems, respectively.

Phase diagrams of exciton-polaritons in different materials Solid lines show the critical concentration Nc versus temperature of the polariton KT phase transition. Dotted and dashed lines show the critical concentration Nc for quasi condensation in 100 µm and 1 meter lateral size systems, respectively.

Trappola in k space per polaritoni

CdTe T=5K

GaN Polaritons at T=300K

BEC in GaN @ 300K

Polariton laser

Laser history... 1917 Einstein derived the Plank formula, spontaneous + stimulated emission 1950 W. Lamb: idea of light amplification 1950 A. Kastler, optical pumping 1953 Weber, Twones, Basov, Prokhorov, maser 1959 T.H.Maiman, laser on rubis 1960s gaz lasers 1969 first semiconductor lasers (pn-junction) 1972 Zh. Alferov, laser on heterostructures 1990s lasers on semiconductor nanostructures, VCSELs 1996, Imamoglou, idea of polariton lasing 2007, RT polariton laser

To make a polariton laser one should have a microcavity in the strong-coupling regime Coherent spontaneous emission from polariton BEC Optically or electronically excited exciton-polaritons relax towards the ground state and Bose-condense there. Their relaxation is stimulated by final state population. The condensate emits spontaneously a coherent light

Escape of polaritons from cavity