Isotopes of boron

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Isotopes of boron

Boron (5B) naturally occurs as isotopes 10
B
and 11
B
, 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 8
B
, with a half-life of only 771.9(9) ms and 12
B
with a half-life of 20.20(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 7
B
and 9
B
) while those with mass above 11 mostly become carbon.

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A chart showing the abundances of the naturally occurring isotopes of boron.

Quick Facts Main isotopes, Decay ...
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)
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List of isotopes

More information Nuclide, Z ...
Nuclide
[n 1]
Z N Isotopic mass (Da)[3]
[n 2][n 3]
Half-life[4]

[resonance width]
Decay
mode
[4]
[n 4]
Daughter
isotope

[n 5]
Spin and
parity[4]
[n 6][n 7]
Natural abundance (mole fraction)
Excitation energy Normal proportion[4] Range of variation
6
B
?[n 8]
5 1 6.050800(2150) p-unstable 2p? 4
Li
?
2−#
7
B
5 2 7.029712(27) 570(14) ys
[801(20) keV]
p 6
Be
[n 9]
(3/2−)
8
B
[n 10][n 11]
5 3 8.0246073(11) 771.9(9) ms β+α 4
He
2+
8m
B
10624(8) keV 0+
9
B
5 4 9.0133296(10) 800(300) zs p 8
Be
[n 12]
3/2−
10
B
[n 13]
5 5 10.012936862(16) Stable 3+ [0.189, 0.204][5]
11
B
5 6 11.009305167(13) Stable 3/2− [0.796, 0.811][5]
11m
B
12560(9) keV 1/2+, (3/2+)
12
B
5 7 12.0143526(14) 20.20(2) ms β (99.40(2)%) 12
C
1+
βα (0.60(2)%) 8
Be
[n 14]
13
B
5 8 13.0177800(11) 17.16(18) ms β (99.734(36)%) 13
C
3/2−
βn (0.266(36)%) 12
C
14
B
5 9 14.025404(23) 12.36(29) ms β (93.96(23)%) 14
C
2−
βn (6.04(23)%) 13
C
β2n ?[n 15] 12
C
 ?
14m
B
17065(29) keV 4.15(1.90) zs IT ?[n 15] 0+
15
B
5 10 15.031087(23) 10.18(35) ms βn (98.7(1.0)%) 14
C
3/2−
β (< 1.3%) 15
C
β2n (< 1.5%) 13
C
16
B
5 11 16.039841(26) > 4.6 zs n ?[n 15] 15
B
 ?
0−
17
B
[n 16]
5 12 17.04693(22) 5.08(5) ms βn (63(1)%) 16
C
(3/2−)
β (21.1(2.4)%) 17
C
β2n (12(2)%) 15
C
β3n (3.5(7)%) 14
C
β4n (0.4(3)%) 13
C
18
B
5 13 18.05560(22) < 26 ns n 17
B
(2−)
19
B
[n 17]
5 14 19.06417(56) 2.92(13) ms βn (71(9)%) 18
C
(3/2−)
β2n (17(5)%) 17
C
β3n (< 9.1%) 16
C
β (> 2.9%) 19
C
20
B
[6]
5 15 20.07451(59) > 912.4 ys n 19
B
(1−, 2−)
21
B
[6]
5 16 21.08415(60) > 760 ys 2n 19
B
(3/2−)
This table header & footer:
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  1. mB  Excited nuclear isomer.
  2. ()  Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
  3. #  Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4. Bold symbol as daughter  Daughter product is stable.
  5. () spin value  Indicates spin with weak assignment arguments.
  6. #  Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  7. This isotope has not yet been observed; given data is inferred or estimated from periodic trends.
  8. Subsequently decays by double proton emission to 4
    He
    for a net reaction of 7
    B
    4
    He
    + 31
    H
  9. Has 1 halo proton
  10. Intermediate product of a branch of proton-proton chain in stellar nucleosynthesis as part of the process converting hydrogen to helium
  11. Immediately decays into two α particles, for a net reaction of 9
    B
    → 24
    He
    + 1
    H
  12. One of the few stable odd-odd nuclei
  13. Immediately decays into two α particles, for a net reaction of 12
    B
    → 34
    He
    + e
  14. Decay mode shown is energetically allowed, but has not been experimentally observed to occur in this nuclide.
  15. Has 2 halo neutrons
  16. Has 4 halo neutrons

Boron-8

Boron-8 is an isotope of boron that undergoes β+ decay to beryllium-8 with a half-life of 771.9(9) ms. It is the strongest candidate for a halo nucleus with a loosely-bound proton, in contrast to neutron halo nuclei such as lithium-11.[7]

Although boron-8 beta decay neutrinos from the Sun make up only about 80 ppm of the total solar neutrino flux, they have a higher energy centered around 10 MeV,[8] and are an important background to dark matter direct detection experiments.[9] 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

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