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Explore the complexities of optical cavities and the role of collective dynamics in light-matter interactions, including concepts like cavity modes, coherent light sources, and master equations. Gain insights into quantum Heisenberg Langevin equations and strong coupling regimes.
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Claudiu Genes Max Planck Institute for the Science of Light (Erlangen, Germany) Lecture 7: Jaynes-Cummings Hamiltonian Laser theory Quantum Physics of Light-Matter Interactions, SS19, FAU
Optical cavities Combining this with complexity – collective dynamics plays a big role
Optical cavity Electric field operator Zero point electric field per photon
Optical cavity Operator creating excitations in a given delocalized mode Electric field operator Zero point electric field per photon
Optical cavity • Multiple resonances • Lorentzian profile – enhanced density of optical modes around resonances Quasi-mode frequency Cavity mode linewidth
Optical cavity Coherent light source
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction 2 equivalent approaches
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Eliminate vacuum modes – master equation for the cavity mode
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Eliminate vacuum modes – master equation for the cavity mode Cavity intensity decay rate
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Eliminate vacuum modes – master equation for the cavity mode Collapse operator
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Eliminate vacuum modes – master equation for the cavity mode
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Eliminate vacuum modes – master equation for the cavity mode Driving field amplitude
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Keep vacuum modes – quantum Heisenberg Langevin equations (quantum stochastic approach)
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction quantum Heisenberg Langevin equations Heisenberg equations of motion and
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction quantum Heisenberg Langevin equations Heisenberg equations of motion and Formal solution
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Effective decay
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Driving plus noise term Effective decay
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Result
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Result Input noise correlations
Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Result Input noise correlations Input-output relations
Cavity quantum electrodynamics Cavity quantum electrodynamics with two-level systems
Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian
Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian
Master equation of cavity-emitter system The full master equation with the total Hamiltonian
Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian Matrix elements
Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian Matrix elements
Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian Matrix elements Up to two excitations
Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian Matrix elements Leads to photon blockade (as we‘ll see later) Up to two excitations
Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace)
Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace) Eigenvalues
Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace) Eigenvalues On resonance
Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace) Eigenvalues On resonance
Atom in cavity- Jaynes Cummings dynamics The polariton transformation Diagonalization of the Hamiltonian Diagonalization of the Linblad term
Master equation of cavity-emitter system The full master equation with the total Hamiltonian
Master equation of cavity-emitter system The full master equation with the total Hamiltonian Let’s derive equations of motion for averages
Master equation of cavity-emitter system The full master equation with the total Hamiltonian Let’s derive equations of motion for averages
Linear regime Low excitation regime: two driven coupled oscillators
Strong coupling Low excitation regime: two driven coupled oscillators • Emergence of strong coupling Decay rates Frequencies
Strong coupling Low excitation regime: two driven coupled oscillators • Emergence of strong coupling
The Purcell effect Bad cavity regime Decay rates Frequencies
The Purcell effect Bad cavity regime Cooperativity (or Purcell factor) Decay rates Frequencies
Photon blockade Photon blockade
The laser Model 1 Fast relaxation pump Lasing transition Incoherent pump
The laser Model 1 Fast relaxation pump Lasing transition Incoherent pump Effective inverse decay – incoherent pumping model ...like decay from the ground to the excited state