Hyperfine interaction in the ground state of the negatively charged nitrogen vacancy center in diamond

By S. Felton, A. Edmonds, M. Newton, P. Martineau, D. Fisher, Daniel J. Twitchen, J. Baker. 2009

214 citations recorded by the source corpus.

Subfields: Electrical and Electronic Engineering, Geophysics, Materials Chemistry

View Paper: https://www.semanticscholar.org/paper/3a634bf1fd8f064f3750fd45201ab16fe70c5a64

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Electrical and Electronic Engineering

1. Á. Gali

In Geophysics

1. M. Turner
2. J. Schloss
3. J. Barry
4. Á. Gali
5. L. Childress
6. R. Walsworth

In Materials Chemistry

1. M. Turner
2. R. Walsworth
3. J. Schloss
4. J. Barry
5. Á. Gali
6. L. Childress
7. C. Hart

Citations in the corpus

• Simultaneous Broadband Vector Magnetometry Using Solid-State Spins (2018, background): “Resonance features numbered 1 - 4 (5 - 8) correspond to |ms = 0〉 → |ms =−1〉 (|ms = 0〉 → |ms = +1〉) spin transitions, and subfeatures arise from NV hyperfine structure [33, 38, 39] (see Supplemental Material and Fig.”
• 13C hyperfine interactions in the nitrogen-vacancy centre in diamond (2011, methodology): “Because the 14N hyperfine interaction is negative in the ground state [11], it polarizes into the highest frequency ESR line; the nearly full polarization of the 14N indicates that its quantization axis is parallel to the NV axis in both the ground and excited states (as expected by symmetry).”
• Production of oriented nitrogen-vacancy color centers in synthetic diamond (2011, unknown): “[4]”