Quantum Maxwell-Bloch equations for spatially inhomogeneous semiconductor lasers
Physical Review A. Atomic, Molecular, and Optical Physics Volume 59 Issue 3
Page 2342-2358
published_at 1999-03
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fulltext
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Title ( eng ) |
Quantum Maxwell-Bloch equations for spatially inhomogeneous semiconductor lasers
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Creator |
Hess Ortwin
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Source Title |
Physical Review A. Atomic, Molecular, and Optical Physics
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Volume | 59 |
Issue | 3 |
Start Page | 2342 |
End Page | 2358 |
Abstract |
We present quantum Maxwell-Bloch equations (QMBE) for spatially inhomogeneous semiconductor laser devices. The QMBE are derived from fully quantum mechanical operator dynamics describing the interaction of the light field with the quantum states of the electrons and the holes near the band gap. By taking into account field-field correlations and field-dipole correlations, the QMBE include quantum noise effects, which cause spontaneous emission and amplified spontaneous emission. In particular, the source of spontaneous emission is obtained by factorizing the dipole-dipole correlations into a product of electron and hole densities. The QMBE are formulated for general devices, for edge emitting lasers and for vertical cavity surface emitting lasers, providing a starting point for the detailed analysis of spatial coherence in the near-field and far-field patterns of such laser diodes. Analytical expressions are given for the spectra of gain and spontaneous emission described by the QMBE. These results are applied to the case of a broad area laser, for which the frequency and carrier density dependent spontaneous emission factor β and the evolution of the far-field pattern near threshold are derived.
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Language |
eng
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Resource Type | journal article |
Publisher |
American Physical Society
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Date of Issued | 1999-03 |
Rights |
Copyright (c) 1999 American Physical Society.
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Publish Type | Version of Record |
Access Rights | open access |
Source Identifier |
[ISSN] 1094-1622
[DOI] 10.1103/PhysRevA.59.2342
[NCID] AA10764867
[DOI] http://dx.doi.org/10.1103/PhysRevA.59.2342
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