Controlling spin relaxation with a cavity

A. Bienfait, J. J. Pla, Y. Kubo, X. Zhou, M. Stern, C. C. Lo, C. D. Weis, T. Schenkel, D. Vion, D. Esteve, J. J. L. Morton and P. Bertet ()
Additional contact information
A. Bienfait: Quantronics Group, SPEC, CEA, CNRS, Université Paris-Saclay, CEA-Saclay
J. J. Pla: London Centre for Nanotechnology, University College London
Y. Kubo: Quantronics Group, SPEC, CEA, CNRS, Université Paris-Saclay, CEA-Saclay
X. Zhou: Quantronics Group, SPEC, CEA, CNRS, Université Paris-Saclay, CEA-Saclay
M. Stern: Quantronics Group, SPEC, CEA, CNRS, Université Paris-Saclay, CEA-Saclay
C. C. Lo: London Centre for Nanotechnology, University College London
C. D. Weis: Lawrence Berkeley National Laboratory
T. Schenkel: Lawrence Berkeley National Laboratory
D. Vion: Quantronics Group, SPEC, CEA, CNRS, Université Paris-Saclay, CEA-Saclay
D. Esteve: Quantronics Group, SPEC, CEA, CNRS, Université Paris-Saclay, CEA-Saclay
J. J. L. Morton: London Centre for Nanotechnology, University College London
P. Bertet: Quantronics Group, SPEC, CEA, CNRS, Université Paris-Saclay, CEA-Saclay

Nature, 2016, vol. 531, issue 7592, 74-77

Abstract: By coupling donor spins in silicon to a superconducting microwave cavity and tuning the spins to the cavity resonance, the rate of spin relaxation is increased by three orders of magnitude compared to that of detuned spins; in such a regime, spontaneous emission of radiation is the dominant mechanism of spin relaxation.

Date: 2016
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DOI: 10.1038/nature16944

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