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Isotopes of boron

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Isotopes of boron (5B)
Main isotopes Decay
abun­dance half-life (t1/2) mode pro­duct
8B synth 771.9 ms β+ 8Be
10B [18.9%, 20.4%] stable
11B [79.6%, 81.1%] stable
Standard atomic weight Ar°(B)

Boron (5B) naturally occurs as isotopes 10B and 11B, the latter of which makes up about 80% of natural boron. There are 14 radioisotopes that have been discovered, with mass numbers from 6 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.

List of isotopes

nuclide
symbol
Z(p) N(n)  
isotopic mass (u)
 
half-life
[resonance width]
decay mode(s)[3] daughter
isotope(s)
nuclear
spin and
parity
representative
isotopic
composition
(mole fraction)
range of natural
variation
(mole percent)
6B 5 1 6.04681(75)#
7B 5 2 7.02992(8) 350(50) × 10−24 s
[1.4(2) MeV]
p 6
Be
[n 1]
(3/2−)
8B[n 2] 5 3 8.0246072(11) 770(3) ms β+, α 2 4
He
2+
9B 5 4 9.0133288(11) 80(30)×10−21 s
[0.54(21) keV]
p, α 8
Be
[n 3]
32
10B 5 5 10.0129370(4) Stable 3+ 0.199(7) 18.929–20.386
11B 5 6 11.0093054(4) Stable 3/2 0.801(7) 79.614–81.071
12B 5 7 12.0143521(15) 20.20(2) ms β (98.4%) 12
C
1+
β, α (1.6%) 8
Be
[n 4]
13B 5 8 13.0177802(12) 17.33(17) ms β (99.72%) 13
C
3/2
β, n (0.279%) 12
C
14B 5 9 14.025404(23) 12.5(5) ms β (93.96%) 14
C
2−
β, n (6.04%) 13
C
15B 5 10 15.031103(24) 9.87(7) ms β, n (93.6%) 14
C
3/2
β (6.0%) 15
C
β, 2n (0.40%) 13
C
16B 5 11 16.03981(6) < 190 × 10−12 s
[< 0.1 MeV]
n 15
B
0−
17B[n 5] 5 12 17.04699(18) 5.08(5) 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 (0.40%) 13
C
18B 5 13 18.05617(86)# < 26 ns n 17
B
(4−)#
19B[n 5] 5 14 19.06373(43)# 2.92(13) ms β 19
C
(3/2−)#
  1. ^ Subsequently decays by double proton emission to 4He for a net reaction of 7B → 4He + 3 1H
  2. ^ Has 1 halo proton
  3. ^ immediately decays into two α particles, for a net reaction of 9B → 2 4He + 1H
  4. ^ Immediately decays into two α particles, for a net reaction of 12B → 3 4He + e
  5. ^ a b Has 2 halo neutrons

Notes

  • The precision of the isotope abundances and atomic mass is limited through variations. The given ranges should be applicable to any normal terrestrial material.
  • Commercially available materials may have been subjected to an undisclosed or inadvertent isotopic fractionation. Substantial deviations from the given mass and composition can occur.
  • Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
  • Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC, which use folical uncertainties.[4]
  • Nuclide masses are given by IUPAP Commission on Symbols, Units, Nomenclature, Atomic Masses and Fundamental Constants (SUNAMCO).
  • Isotope abundances are given by IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW).
  • Neutrinos from Boron-8 beta decays within the sun are an important background to dark matter direct detection experiments.[5] 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 (BNCT) as an experimental treatment of some brain cancers.

References

Notes

  1. ^ "Standard Atomic Weights: Boron". CIAAW. 2009.
  2. ^ Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.
  3. ^ "Universal Nuclide Chart". nucleonica. {{cite web}}: Unknown parameter |registration= ignored (|url-access= suggested) (help)
  4. ^ "2.5.7. Standard and expanded uncertainties". Engineering Statistics Handbook. Retrieved 2010-09-16.
  5. ^ 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 (05): 118. arXiv:1604.01025. Bibcode:2016JHEP...05..118C. doi:10.1007/JHEP05(2016)118.

General references