Author
Listed:
- Leon C. Camenzind
(University of Basel)
- Liuqi Yu
(University of Basel)
- Peter Stano
(RIKEN
University of Tokyo
Slovak Academy of Sciences)
- Jeramy D. Zimmerman
(University of California
Colorado School of Mines)
- Arthur C. Gossard
(University of California)
- Daniel Loss
(University of Basel
RIKEN)
- Dominik M. Zumbühl
(University of Basel)
Abstract
Understanding and control of the spin relaxation time T1 is among the key challenges for spin-based qubits. A larger T1 is generally favored, setting the fundamental upper limit to the qubit coherence and spin readout fidelity. In GaAs quantum dots at low temperatures and high in-plane magnetic fields B, the spin relaxation relies on phonon emission and spin–orbit coupling. The characteristic dependence T1 ∝ B−5 and pronounced B-field anisotropy were already confirmed experimentally. However, it has also been predicted 15 years ago that at low enough fields, the spin–orbit interaction is replaced by the coupling to the nuclear spins, where the relaxation becomes isotropic, and the scaling changes to T1 ∝ B−3. Here, we establish these predictions experimentally, by measuring T1 over an unprecedented range of magnetic fields—made possible by lower temperature—and report a maximum T1 = 57 ± 15 s at the lowest fields, setting a record electron spin lifetime in a nanostructure.
Suggested Citation
Leon C. Camenzind & Liuqi Yu & Peter Stano & Jeramy D. Zimmerman & Arthur C. Gossard & Daniel Loss & Dominik M. Zumbühl, 2018.
"Hyperfine-phonon spin relaxation in a single-electron GaAs quantum dot,"
Nature Communications, Nature, vol. 9(1), pages 1-6, December.
Handle:
RePEc:nat:natcom:v:9:y:2018:i:1:d:10.1038_s41467-018-05879-x
DOI: 10.1038/s41467-018-05879-x
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