The following table lists the magnetic properties at higher field strengths required for choosing the nuclei to be used in NMR experiments. The table shows NMR frequency at the indicated field strength for a variety of isotopes. The reader is referred to several excellent texts and the literature for guidelines in nucleus selection (Refs. 1–15) . For more detailed information on these and other less common nuclei at 10 kG, the reader should consult the table entitled "Nuclear Spins, Moments, and Other Data Related to NMR Spectroscopy" in this section. Column definitions for the table are as follows.
Column heading | Definition |
Isotope | Atomic symbol for isotope |
Abundance | Isotopic abundance (fractional) on Earth |
Spin I | Nuclear spin |
10.000 kG, 14.092 kG, etc. | NMR frequency at magnetic field specified, in MHz |
Isotope | Abundance | Spin I | 10.000 kG | 14.092 kG | 21.139 kG | 23.487 kG | 51.567 kG | 93.950 kG | 140.925 kG | 223.131 kG |
11H | [0.999 72, 0.999 99] | 1/2 | 42.5759 | 60.0000 | 90.0000 | 100.0000 | 220.0000 | 400.0000 | 600.0000 | 950.0000 |
21H | [0.000 01, 0.000 28] | 1 | 6.53566 | 9.21037 | 13.81555 | 15.35061 | 33.77134 | 61.40262 | 92.10380 | 145.9830 |
31H* | 1/2 | 45.4129 | 63.9980 | 95.9971 | 106.6634 | 234.6595 | 426.6542 | 639.9813 | 1013.3024 | |
136C | [0.0096, 0.0116] | 1/2 | 10.7054 | 15.0866 | 22.6298 | 25.1443 | 55.3174 | 100.5735 | 150.8659 | 2388.5150 |
147N | [0.995 78, 0.996 63] | 1 | 3.0756 | 4.3343 | 6.5014 | 7.2238 | 15.924 | 28.9104 | 43.3615 | 68.6557 |
157N | [0.003 37, 0.004 22] | 1/2 | 4.3142 | 6.0798 | 9.1197 | 10.1330 | 22.2925 | 40.5306 | 60.7960 | 96.2601 |
178O | [0.000 367, 0.000 400] | 5/2 | 5.772 | 8.134 | 12.201 | 13.557 | 29.825 | 54.1811 | 81.3186 | 128.5801 |
199F | 1 | 1/2 | 40.0541 | 42.3537 | 63.5305 | 94.0769 | 206.9692 | 376.2515 | 564.3781 | 893.5963 |
2914Si | [0.046 45, 0.046 99] | 1/2 | 8.4578 | 11.9191 | 17.8787 | 19.8652 | 43.7035 | 79.4638 | 119.1956 | 188.72 |
3115P | 1 | 1/2 | 17.235 | 24.288 | 36.433 | 40.481 | 89.057 | 161.9828 | 242.9741 | 384.7086 |
3316S | [0.007 29, 0.007 97] | 3/2 | 3.2654 | 4.6018 | 6.9026 | 7.6696 | 16.8731 | 30.6826 | 46.0238 | 72.8710 |
3516S* | 3/2 | 5.08 | 7.16 | 10.74 | 11.932 | 26.250 | 47.7267 | 71.5875 | 113.3508 | |
3517Cl | [0.755, 0.761] | 3/2 | 4.1717 | 5.8790 | 8.8184 | 9.7983 | 21.5562 | 39.1948 | 58.7902 | 93.0876 |
3617Cl* | 2 | 4.8931 | 6.8956 | 10.3434 | 11.4927 | 25.2838 | 45.9638 | 68.9432 | 109.1639 | |
7635Br* | 1 | 4.18 | 5.89 | 8.84 | 9.82 | 21.60 | 39.2768 | 58.9130 | 93.2822 | |
7935Br | [0.505, 0.508] | 3/2 | 10.667 | 15.032 | 22.549 | 25.054 | 55.119 | 100.2133 | 150.3202 | 238.0064 |
8135Br | [0.492, 0.495] | 3/2 | 11.498 | 16.204 | 24.305 | 27.006 | 59.413 | 108.0258 | 162.0386 | 256.5608 |
18374W | 0.1431(4) | 1/2 | 1.7716 | 2.4966 | 3.7449 | 4.1610 | 9.1543 | 16.6430 | 24.9646 | 39.5272 |
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