Nitrogen-vacancy center in diamond: Model of the electronic structure and associated dynamics
By N. Manson, J. Harrison, Matthew J. Sellars. 2006
547 citations recorded by the source corpus.
Subfields: Electrical and Electronic Engineering, Geophysics, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/912d13db6dafcc9cb9e44abcc2b455e6bcbfdfec
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In Electrical and Electronic Engineering
- David D. Awschalom
- N. Manson
- A. Janotti
- J. Cardenas
- Ronald Hanson
- Audrius Alkauskas
- G. Burkard
- Michal Lipson
In Geophysics
In Materials Chemistry
- R. Walsworth
- David D. Awschalom
- Ronald Hanson
- Á. Gali
- L. Pham
- Daniel J. Twitchen
- Fedor Jelezko
- N. Manson
Citations in the corpus
- Measurement and Control of Single Nitrogen-Vacancy Center Spins above 600 K (2012, methodology): “tected ESR signal observed in experiment [8].”
- A quantum memory intrinsic to single nitrogen-vacancy centres in diamond (2011, methodology): “After optically polarizing the electronic spin into m s =0 (refs&nbs”
- Infrared emission of the NV centre in diamond: Zeeman and uniaxial stress studies (2008, methodology): “The ex ited state is split by diagonal spin-orbit intera tion λLzSz into threeequally spa ed doubly degenerate levels and there are small displa ements from thenon-diagonal spin-orbit intera tion, λ (L+S− + L−S+) [12℄.”
- Magnetic field imaging with nitrogen-vacancy ensembles (2011, background): “These transitions are primarily spin conserving; however, there exists an alternative decay path that transfers approximately 30% of the ms = ±1 excited state population to the ms = 0 ground state through a metastable singlet state [9, 10], without emitting a photon in the fluorescence band.”
- Diamond-based single-photon emitters (2011, background): “Since the NV− center has an even number of electrons and C3ν symmetry, group theory states that the many-electron configuration forms spin triplet states ((3)A2 and 3E), and spin singlet states (1E and (1)A1) [62].”
- Spin-flip and spin-conserving optical transitions of the nitrogen-vacancy centre in diamond (2008, background): “the states associated with Sx and Sy spins (((3)E)(A1, A2)) and (3E)E by λ〈E ‖ L (A2) ‖ E〉 = a and−a, respectively, and from a six electron (two hole) model a is considered to be positive [9].”