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Quantum Physics of Light-Matter Interactions, SS19, FAU

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.

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Quantum Physics of Light-Matter Interactions, SS19, FAU

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  1. 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

  2. Optical cavities Combining this with complexity – collective dynamics plays a big role

  3. Optical cavity

  4. Optical cavity Electric field operator Zero point electric field per photon

  5. Optical cavity Operator creating excitations in a given delocalized mode Electric field operator Zero point electric field per photon

  6. Optical cavity • Multiple resonances • Lorentzian profile – enhanced density of optical modes around resonances Quasi-mode frequency Cavity mode linewidth

  7. Optical cavity Coherent light source

  8. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction 2 equivalent approaches

  9. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Eliminate vacuum modes – master equation for the cavity mode

  10. 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

  11. 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

  12. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Eliminate vacuum modes – master equation for the cavity mode

  13. 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

  14. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Keep vacuum modes – quantum Heisenberg Langevin equations (quantum stochastic approach)

  15. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction quantum Heisenberg Langevin equations Heisenberg equations of motion and

  16. 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

  17. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction

  18. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Effective decay

  19. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Driving plus noise term Effective decay

  20. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Result

  21. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Result Input noise correlations

  22. Optical cavity Coherent light source Leakage of cavity photons modelled as an exchange interaction Result Input noise correlations Input-output relations

  23. Cavity quantum electrodynamics Cavity quantum electrodynamics with two-level systems

  24. Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian

  25. Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian

  26. Master equation of cavity-emitter system The full master equation with the total Hamiltonian

  27. Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian Matrix elements

  28. Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian Matrix elements

  29. Atom in cavity- Jaynes Cummings dynamics The Jaynes-Cummings Hamiltonian Matrix elements Up to two excitations

  30. 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

  31. Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace)

  32. Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace) Eigenvalues

  33. Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace) Eigenvalues On resonance

  34. Atom in cavity- Jaynes Cummings dynamics Polaritons (single excitation subspace) Eigenvalues On resonance

  35. Atom in cavity- Jaynes Cummings dynamics The polariton transformation Diagonalization of the Hamiltonian Diagonalization of the Linblad term

  36. Master equation of cavity-emitter system The full master equation with the total Hamiltonian

  37. Master equation of cavity-emitter system The full master equation with the total Hamiltonian Let’s derive equations of motion for averages

  38. Master equation of cavity-emitter system The full master equation with the total Hamiltonian Let’s derive equations of motion for averages

  39. Linear regime Low excitation regime: two driven coupled oscillators

  40. Strong coupling Low excitation regime: two driven coupled oscillators • Emergence of strong coupling Decay rates Frequencies

  41. Strong coupling Low excitation regime: two driven coupled oscillators • Emergence of strong coupling

  42. The Purcell effect Bad cavity regime Decay rates Frequencies

  43. The Purcell effect Bad cavity regime Cooperativity (or Purcell factor) Decay rates Frequencies

  44. Photon blockade Photon blockade

  45. Photon blockade

  46. Photon blockade

  47. The laser (quantum theory)

  48. Source: youtube: How a laser works

  49. The laser Model 1 Fast relaxation pump Lasing transition Incoherent pump

  50. 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

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