Isotopes of boron
Boron (5B) naturally occurs as isotopes 10B and 11B, the latter of which makes up about 80% of natural boron. There are 13 radioisotopes that have been discovered, with mass numbers from 7 to 21, all with short half-lives, the longest being that of 8B, with a half-life of only 770 milliseconds (ms) and 12B with a half-life of 20.2 ms. All other isotopes have half-lives shorter than 17.35 ms. Those isotopes with mass below 10 decay into helium (via short-lived isotopes of beryllium for 7B and 9B) while those with mass above 11 mostly become carbon.

A chart showing the abundances of the naturally occurring isotopes of boron.
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| Standard atomic weight Ar, standard(B) | [10.806, 10.821] conventional: 10.81[2][3] | |||||||||||||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
List of isotopes
| Nuclide[4] [n 1] |
Z | N | Isotopic mass (Da)[5] [n 2][n 3] |
Half-life [resonance width] |
Decay mode [n 4] |
Daughter isotope [n 5] |
Spin and parity [n 6][n 7] |
Natural abundance (mole fraction) | |||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Excitation energy | Normal proportion | Range of variation | |||||||||||||||||
| 7B | 5 | 2 | 7.029712000±0.000027000 | 570±14 ys [801(20) keV] | p | 6 Be [n 8] |
(3/2−) | ||||||||||||
| 8B[n 9] | 5 | 3 | 8.024607315±0.000001073 | 771.9±0.9 ms | β+, α | 2 4 He |
2+ | ||||||||||||
| 9B | 5 | 4 | 9.013329645±0.000000969 | 800±300 zs [0.54(21) keV] | p, α | 2 4 He |
3/2− | ||||||||||||
| 10B[n 10] | 5 | 5 | 10.012936862±0.000000016 | Stable | 3+ | [0.189, 0.204][6] | |||||||||||||
| 11B | 5 | 6 | 11.009305166±0.000000013 | Stable | 3/2− | [0.796, 0.811][6] | |||||||||||||
| 12B | 5 | 7 | 12.014352638±0.000001418 | 20.20±0.02 ms | β− (98.4%) | 12 C |
1+ | ||||||||||||
| β−, α (1.6%) | 8 Be [n 11] | ||||||||||||||||||
| 13B | 5 | 8 | 13.017779981±0.000001073 | 17.16±0.18 ms | β− (99.72%) | 13 C |
3/2− | ||||||||||||
| β−, n (0.28%) | 12 C | ||||||||||||||||||
| 14B | 5 | 9 | 14.025404010±0.000022773 | 12.36±0.29 ms | β− (93.96%) | 14 C |
2− | ||||||||||||
| β−, n (6.04%) | 13 C | ||||||||||||||||||
| 15B | 5 | 10 | 15.031087023±0.000022575 | 10.18±0.35 ms | β−, n (93.6%) | 14 C |
3/2− | ||||||||||||
| β− (6.0%) | 15 C | ||||||||||||||||||
| β−, 2n (0.4%) | 13 C | ||||||||||||||||||
| 16B | 5 | 11 | 16.039841045±0.000026373 | >4.6 zs | n | 15 B |
0− | ||||||||||||
| 17B[n 12] | 5 | 12 | 17.046931399±0.000219114 | 5.08±0.05 ms | β−, n (63.0%) | 16 C |
(3/2−) | ||||||||||||
| β− (22.1%) | 17 C | ||||||||||||||||||
| β−, 2n (11.0%) | 15 C | ||||||||||||||||||
| β−, 3n (3.5%) | 14 C | ||||||||||||||||||
| β−, 4n (0.4%) | 13 C | ||||||||||||||||||
| 18B | 5 | 13 | 18.055601683±0.000219180 | <26 ns | n | 17 B |
(2−) | ||||||||||||
| 19B[n 12] | 5 | 14 | 19.064166000±0.000564000 | 2.92±0.13 ms | β−, n (71%) | 18 C |
3/2−# | ||||||||||||
| β−, 2n (17%) | 17 C | ||||||||||||||||||
| β− (12%) | 19 C | ||||||||||||||||||
| 20B[7] | 5 | 15 | 20.074505644±0.000586538 | >912.4 ys | n | 19 B |
(1−, 2−) | ||||||||||||
| 21B[7] | 5 | 16 | 21.084147485±0.000599750 | <760 ys [2.47(19) MeV] | 2n | 19 B |
(3/2−)# | ||||||||||||
| This table header & footer: | |||||||||||||||||||
- mB – Excited nuclear isomer.
- ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
- # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
-
Modes of decay:
n: Neutron emission p: Proton emission - Bold symbol as daughter – Daughter product is stable.
- ( ) spin value – Indicates spin with weak assignment arguments.
- # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
- Subsequently decays by double proton emission to 4He for a net reaction of 7B → 4He + 3 1H
- Has 1 halo proton
- One of the few stable odd-odd nuclei
- Immediately decays into two α particles, for a net reaction of 12B → 3 4He + e−
- Has 2 halo neutrons
- Neutrinos from boron-8 beta decays within the sun are an important background to dark matter direct detection experiments.[8] They are the first component of the neutrino floor that dark matter direct detection experiments are expected to eventually encounter.
Applications
Boron-10
Boron-10 is used in boron neutron capture therapy as an experimental treatment of some brain cancers.
References
- "Atomic Weight of Boron". CIAAW. Retrieved 2021-10-26.
- "Standard Atomic Weights: Boron". CIAAW. 2009.
- Meija, Juris; et al. (2016). "Atomic weights of the elements 2013 (IUPAC Technical Report)". Pure and Applied Chemistry. 88 (3): 265–91. doi:10.1515/pac-2015-0305.
- Half-life, decay mode, nuclear spin, and isotopic composition is sourced in:
Kondev, F.G.; Wang, M.; Huang, W.J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae. - Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3): 030003. doi:10.1088/1674-1137/abddaf.
- "Atomic Weight of Boron". CIAAW.
- Leblond, S.; et al. (2018). "First observation of 20B and 21B". Physical Review Letters. 121 (26): 262502–1–262502–6. arXiv:1901.00455. doi:10.1103/PhysRevLett.121.262502. PMID 30636115.
- Cerdeno, David G.; Fairbairn, Malcolm; Jubb, Thomas; Machado, Pedro; Vincent, Aaron C.; Boehm, Celine (2016). "Physics from solar neutrinos in dark matter direct detection experiments". JHEP. 2016 (5): 118. arXiv:1604.01025. Bibcode:2016JHEP...05..118C. doi:10.1007/JHEP05(2016)118.
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