2018
DOI: 10.1103/physrevlett.120.257401
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Phonon Decoherence of Quantum Dots in Photonic Structures: Broadening of the Zero-Phonon Line and the Role of Dimensionality

Abstract: We develop a general microscopic theory describing the phonon decoherence of quantum dots and indistinguishability of the emitted photons in photonic structures. The coherence is found to depend fundamentally on the dimensionality of the structure resulting in vastly different performance for quantum dots embedded in a nanocavity (0D), waveguide (1D), slab (2D), or bulk medium (3D). In bulk, we find a striking temperature dependence of the dephasing rate scaling as T^{11} implying that phonons are effectively … Show more

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Cited by 65 publications
(69 citation statements)
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“…is the pure-dephasing rate due to the virtual phonon scattering [47,49]. Using this expression, the final master equation becomes…”
Section: Appendix B: Rabi Oscillation Master Equationmentioning
confidence: 99%
“…is the pure-dephasing rate due to the virtual phonon scattering [47,49]. Using this expression, the final master equation becomes…”
Section: Appendix B: Rabi Oscillation Master Equationmentioning
confidence: 99%
“…The successful interference relies on highly coherent and indistinguishable single photons, which requires a sufficiently long coherence time compared to the spontaneous decay time , that is 2 . However, the existence of phonon interactions and charge fluctuations in the solidstate environment causes timing and spectral jitters as well as pure dephasing, and thus the emitters have a broad emission linewidth compared to their intrinsic linewidth limited by the lifetime [117]. Such linewidth broadening is worse with an above-band excitation scheme that increases unnecessary interactions in solid-state systems.…”
Section: A Coherent Control Of Quantum Emittersmentioning
confidence: 99%
“…The calculation of the ID follows the derivations of Reference [27] and the key results are summarized below. The interaction between a QD exciton and an acoustic phonon mode is well described by the electron-phonon deformation-potential interaction [17,25,27,31], which characterizes the effects on the bandstructure due to strain. We assume that at low temperatures only the exciton ground state |ψ 1 is populated.…”
Section: Theory Of the Exciton-phonon Interaction And Numerical Modelmentioning
confidence: 99%
“…For QDs in a homogeneous material (bulk), the phonon sideband and the broadening of the ZPL can be explained by a linear (absorption and emission of phonons) and quadratic exciton-phonon coupling (elastic scattering processes), respectively [17,23,24,25]. In photonic nanostructures, the picture is more involved and additional linear contributions to the broadening of the ZPL have been identified [26,27], which constitute the dominant dephasing mechanism at low temperatures. The sideband photons may readily and efficiently be removed by spectral filtering.…”
Section: Introductionmentioning
confidence: 99%
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