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. 2022 Dec 6;13:7501. doi: 10.1038/s41467-022-35048-0

Table 2.

Calculated hyperfine tensors for NCVC−1 in diamond, CBVN in hBN, and WSe in MoSe2

Hosts Defects Nuclear spins Number of equivalent sites Hyperfine tensors (MHz) (convention: |Azz| > |Axx| > |Ayy|)
Axx Ayy Azz
Diamond NCVC−1 14N (I = 1, 99.632%) 1 −2.9 −2.6 −2.9
15N (I = 1/2, 0.368%) 1 4.1 3.6 4.1
13C (I = 1/2, 1.07%) 3 145.0 144.8 227.2
13C (I = 1/2, 1.07%) 6 14.2 14.1 19.9
hBN CBVN 13C (I = 1/2, 1.07%) 1 474.7 400.9 478.8
10B (I = 3, 19.9%) 1 24.9 22.2 26.4
11B (I = 3/2, 80.1%) 2 74.4 66.3 78.9
14N (I = 1, 99.632%) 2 7.3 7.2 9.9
15N (I = 1/2, 0.368%) 2 −10.3 −10.1 −13.9
MoSe2 WSe 183W (I = 1/2, 14.31%) 1 332.9 253.0 333.0
95Mo (I = 5/2, 15.92%) 3 14.6 8.4 16.5
97Mo (I = 5/2, 9.55%) 3 14.9 8.6 16.8
77Se (I = 1/2, 7.63%) 6 68.2 65.4 78.2

The nuclear spin quantum number I and natural abundance are displayed in the nuclear spins column.