Book contents
- Frontmatter
- Contents
- Preface
- 1 Central concepts in classical mechanics
- 2 Central concepts in classical electromagnetism
- 3 Central concepts in quantum mechanics
- 4 Central concepts in stationary quantum theory
- 5 Central concepts in measurement theory
- 6 Wigner's phase-space representation
- 7 Hamiltonian formulation of classical electrodynamics
- 8 System Hamiltonian of classical electrodynamics
- 9 System Hamiltonian in the generalized Coulomb gauge
- 10 Quantization of light and matter
- 11 Quasiparticles in semiconductors
- 12 Band structure of solids
- 13 Interactions in semiconductors
- 14 Generic quantum dynamics
- 15 Cluster-expansion representation of the quantum dynamics
- 16 Simple many-body systems
- 17 Hierarchy problem for dipole systems
- 18 Two-level approximation for optical transitions
- 19 Self-consistent extension of the two-level approach
- 20 Dissipative extension of the two-level approach
- 21 Quantum-optical extension of the two-level approach
- 22 Quantum dynamics of two-level system
- 23 Spectroscopy and quantum-optical correlations
- 24 General aspects of semiconductor optics
- 25 Introductory semiconductor optics
- 26 Maxwell-semiconductor Bloch equations
- 27 Coherent vs. incoherent excitons
- 28 Semiconductor luminescence equations
- 29 Many-body aspects of excitonic luminescence
- 30 Advanced semiconductor quantum optics
- Appendix Conservation laws for the transfer matrix
- Index
- References
30 - Advanced semiconductor quantum optics
Published online by Cambridge University Press: 05 January 2012
- Frontmatter
- Contents
- Preface
- 1 Central concepts in classical mechanics
- 2 Central concepts in classical electromagnetism
- 3 Central concepts in quantum mechanics
- 4 Central concepts in stationary quantum theory
- 5 Central concepts in measurement theory
- 6 Wigner's phase-space representation
- 7 Hamiltonian formulation of classical electrodynamics
- 8 System Hamiltonian of classical electrodynamics
- 9 System Hamiltonian in the generalized Coulomb gauge
- 10 Quantization of light and matter
- 11 Quasiparticles in semiconductors
- 12 Band structure of solids
- 13 Interactions in semiconductors
- 14 Generic quantum dynamics
- 15 Cluster-expansion representation of the quantum dynamics
- 16 Simple many-body systems
- 17 Hierarchy problem for dipole systems
- 18 Two-level approximation for optical transitions
- 19 Self-consistent extension of the two-level approach
- 20 Dissipative extension of the two-level approach
- 21 Quantum-optical extension of the two-level approach
- 22 Quantum dynamics of two-level system
- 23 Spectroscopy and quantum-optical correlations
- 24 General aspects of semiconductor optics
- 25 Introductory semiconductor optics
- 26 Maxwell-semiconductor Bloch equations
- 27 Coherent vs. incoherent excitons
- 28 Semiconductor luminescence equations
- 29 Many-body aspects of excitonic luminescence
- 30 Advanced semiconductor quantum optics
- Appendix Conservation laws for the transfer matrix
- Index
- References
Summary
The discussions in the previous chapters show that already the spontaneous emission, i.e., the simplest manifestation of the quantum-optical fluctuations, exhibits highly nontrivial features as soon as the quantum light is coupled to interacting many-body systems. We have seen, for example, that pronounced resonances in the semiconductor luminescence originate from a nontrivial mixture of exciton and plasma contributions in contrast to the simple transitions between the eigenstates of isolated atomic systems. As a consequence of the conservation laws inherent to the light–matter coupling, the photon emission induces rearrangements in the entire many-body system leading, e.g., to pronounced hole burning in the exciton distribution. As discussed in Chapter 29, this depletion of the optically active excitons leads to a reduction of the total radiative recombination and the appearance of nonthermal luminescence even when the electron–hole system is in quasiequilibrium. Already these observations show that the coupled quantum-optical and many-body interactions induce new intriguing phenomena that are not explainable by the concepts of traditional quantum optics or classical semiconductor physics alone.
The foundations of quantum optics are based on systematic investigations of simple systems interacting with few quantized light modes. In this context, one can evaluate and even measure the exact eigenstates or the density matrix with respect to both the photonic and the atomic degrees of freedom. In semiconductor systems, currently the investigations using one or a few quantum dots (QD) are closest to the atomic studies because, due to their discrete eigenstates, one can treat strongly confined quantum dots to some extent like artificial atoms.
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- Information
- Semiconductor Quantum Optics , pp. 608 - 626Publisher: Cambridge University PressPrint publication year: 2011