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Physically motivated analytical expression for the temperature dependence of the zero-field splitting of the nitrogen-vacancy center in diamond

M. C. Cambria1, G. Thiering2, A. Norambuena3, H. T. Dinani4, A. Gardill1, I. Kemeny1, V. Lordi5, Á. Gali2,6, J. R. Maze7,8 et al.

S. Kolkowitz1,9,*

  • 1Department of Physics, University of Wisconsin, Madison, Wisconsin 53706, USA
  • 2HUN-REN Wigner Research Centre for Physics, P.O. Box 49, 1525 Budapest, Hungary
  • 3Centro de Optica e Información Cuántica, Universidad Mayor, Camino la Piramide 5750, Huechuraba, Santiago, Chile
  • 4Escuela de Ingeniería, Facultad de Ciencias, Ingeniería y Tecnología, Universidad Mayor, Santiago, Chile
  • 5Lawrence Livermore National Laboratory, Livermore, California 94551, USA
  • 6Department of Atomic Physics, Institute of Physics, Budapest University of Technology and Economics, Műegyetem rakpart 3, 1111 Budapest, Hungary
  • 7Instituto de Física, Pontificia Universidad Católica de Chile, Casilla 306, Santiago, Chile
  • 8Centro de Investigación en Nanotecnología y Materiales Avanzados, Pontificia Universidad Católica de Chile, Santiago, Chile
  • 9Department of Physics, University of California, Berkeley, California 94720, USA

  • *kolkowitz@berkeley.edu

Phys. Rev. B 108, L180102 – Published 8 November, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L180102

Abstract

The temperature dependence of the zero-field splitting (ZFS) between the |ms=0〉 and |ms=±1〉 levels of the nitrogen-vacancy (NV) center's electronic ground-state spin triplet can be used as a robust nanoscale thermometer in a broad range of environments. However, despite numerous measurements of this dependence in different temperature ranges, to our knowledge no analytical expression has been put forward that captures the scaling of the ZFS of the NV center across all relevant temperatures. Here we present a simple, analytical, and physically motivated expression for the temperature dependence of the NV center's ZFS that matches all experimental observations, in which the ZFS shifts in proportion to the occupation numbers of two representative phonon modes. In contrast to prior models our expression does not diverge outside the regions of fitting. We show that our model quantitatively matches experimental measurements of the ZFS from 15 to 500 K in single NV centers in ultrapure bulk diamond, and we compare our model and measurements to prior models and experimental data.

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