Long-time coherence in fourth-order spin correlation functions
arXiv:1705.03712 · doi:10.1103/PhysRevB.96.045441
Abstract
We study the long-time decay of fourth-order electron spin correlation functions for an isolated singly charged semi-conductor quantum dot. The electron spin dynamics is governed by the applied external magnetic field as well as the hyperfine interaction. While the long-time coherent oscillations in the correlation functions can be understood within an semi-classical approach treating the Overhauser field as frozen, the field dependent decay of its amplitude reported in different experiments cannot be explained by the central-spin model indicating the insufficiency of such a description. By incorporating the nuclear Zeeman splitting and the strain induced nuclear-electric quadrupolar interaction, we find the correct crossover from a fast decay in small magnetic fields to a slow exponential asymptotic in large magnetic fields. It originates from a competition between the quadrupolar interaction inducing an enhanced spin decay and the nuclear Zeeman term that suppressed the spin-flip processes. We are able to explain the magnetic field dependency of the characteristic long-time decay time depending on the experimental setups. The calculated asymptotic values of s agree qualitatively well with the experimental data.
13 pages, 9 figures
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Cited by in corpus (10)
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- Quench dynamics of spin in quantum dots coupled to spin-polarized leads
- Nuclear Spin Noise in the Central Spin Model
- Interplay of spin mode locking and nuclei-induced frequency focusing in quantum dots
- Quantum mechanical treatment of large spin baths
- Cross-correlation spectra in interacting quantum dot systems
- Signatures of long-range spin-spin interactions in an (In,Ga)As quantum dot ensemble
- Fourth-order spin correlation function in the extended central spin model