Erratum: State-selective intersystem crossing in nitrogen-vacancy centers [Phys. Rev. B 91, 165201 (2015)]

Erratum: State-selective intersystem crossing in nitrogen-vacancy centers [Phys. Rev. B 91,... PHYSICAL REVIEW B 96, 039905(E) (2017) Erratum: State-selective intersystem crossing in nitrogen-vacancy centers [Phys. Rev. B 91, 165201 (2015)] M. L. Goldman, M. W. Doherty, A. Sipahigil, N. Y. Yao, S. D. Bennett, N. B. Manson, A. Kubanek, and M. D. Lukin (Received 6 July 2017; published 25 July 2017) DOI: 10.1103/PhysRevB.96.039905 We have become aware that the vibrational overlap function F (), which is defined in Eq. (5), was incorrectly normalized. This quantity factors into the intersystem crossing (ISC) rates  and  from the states |A  and |E  [Eqs. (6) and (13), A E 1 1,2 1 1,2 respectively]. As a result, the theoretical value of  that is plotted in Fig. 5 is too large by a factor of 2π. We thank A. Gali for bringing this error to our attention. We have also reexamined an assumption regarding the transverse spin-orbit coupling rate λ and found it not to be valid. The dynamic Jahn-Teller effect in the E excited state manifold causes the strengths of the spin-orbit interaction and the excited states’ response to externally applied fields to be reduced [1] by a quantity known as the Ham reduction factor [2]. This factor changes http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Physical Review B American Physical Society (APS)

Erratum: State-selective intersystem crossing in nitrogen-vacancy centers [Phys. Rev. B 91, 165201 (2015)]

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Erratum: State-selective intersystem crossing in nitrogen-vacancy centers [Phys. Rev. B 91, 165201 (2015)]

Abstract

PHYSICAL REVIEW B 96, 039905(E) (2017) Erratum: State-selective intersystem crossing in nitrogen-vacancy centers [Phys. Rev. B 91, 165201 (2015)] M. L. Goldman, M. W. Doherty, A. Sipahigil, N. Y. Yao, S. D. Bennett, N. B. Manson, A. Kubanek, and M. D. Lukin (Received 6 July 2017; published 25 July 2017) DOI: 10.1103/PhysRevB.96.039905 We have become aware that the vibrational overlap function F (), which is defined in Eq. (5), was incorrectly normalized. This quantity factors into the intersystem crossing (ISC) rates  and  from the states |A  and |E  [Eqs. (6) and (13), A E 1 1,2 1 1,2 respectively]. As a result, the theoretical value of  that is plotted in Fig. 5 is too large by a factor of 2π. We thank A. Gali for bringing this error to our attention. We have also reexamined an assumption regarding the transverse spin-orbit coupling rate λ and found it not to be valid. The dynamic Jahn-Teller effect in the E excited state manifold causes the strengths of the spin-orbit interaction and the excited states’ response to externally applied fields to be reduced [1] by a quantity known as the Ham reduction factor [2]. This factor changes
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Publisher
The American Physical Society
Copyright
Copyright © ©2017 American Physical Society
ISSN
1098-0121
eISSN
1550-235X
D.O.I.
10.1103/PhysRevB.96.039905
Publisher site
See Article on Publisher Site

Abstract

PHYSICAL REVIEW B 96, 039905(E) (2017) Erratum: State-selective intersystem crossing in nitrogen-vacancy centers [Phys. Rev. B 91, 165201 (2015)] M. L. Goldman, M. W. Doherty, A. Sipahigil, N. Y. Yao, S. D. Bennett, N. B. Manson, A. Kubanek, and M. D. Lukin (Received 6 July 2017; published 25 July 2017) DOI: 10.1103/PhysRevB.96.039905 We have become aware that the vibrational overlap function F (), which is defined in Eq. (5), was incorrectly normalized. This quantity factors into the intersystem crossing (ISC) rates  and  from the states |A  and |E  [Eqs. (6) and (13), A E 1 1,2 1 1,2 respectively]. As a result, the theoretical value of  that is plotted in Fig. 5 is too large by a factor of 2π. We thank A. Gali for bringing this error to our attention. We have also reexamined an assumption regarding the transverse spin-orbit coupling rate λ and found it not to be valid. The dynamic Jahn-Teller effect in the E excited state manifold causes the strengths of the spin-orbit interaction and the excited states’ response to externally applied fields to be reduced [1] by a quantity known as the Ham reduction factor [2]. This factor changes

Journal

Physical Review BAmerican Physical Society (APS)

Published: Jul 25, 2017

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