Isotopes of silicon

Silicon (14Si) has 23 known isotopes, with mass numbers ranging from 22 to 44. 28Si (the most abundant isotope, at 92.23%), 29Si (4.67%), and 30Si (3.1%) are stable. The longest-lived radioisotope is 32Si, which is produced by cosmic ray spallation of argon. Its half-life has been determined to be approximately 150 years (with decay energy 0.21 MeV), and it decays by beta emission to 32P (which has a 14.27-day half-life) and then to 32S. After 32Si, 31Si has the second longest half-life at 157.3 minutes. All others have half-lives under 7 seconds.



List of isotopes

 * rowspan=3|22Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 8
 * rowspan=3|22.03611(54)#
 * rowspan=3|28.7(11) ms
 * β+, p (62%)
 * 21Mg
 * rowspan=3|0+
 * rowspan=3|
 * rowspan=3|
 * β+ (37%)
 * 22Al
 * β+, 2p (0.7%)
 * 20Na
 * rowspan=3|23Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 9
 * rowspan=3|23.02571(54)#
 * rowspan=3|42.3(4) ms
 * β+, p (88%)
 * 22Mg
 * rowspan=3|3/2+#
 * rowspan=3|
 * rowspan=3|
 * β+ (8%)
 * 23Al
 * β+, 2p (3.6%)
 * 21Na
 * rowspan=2|24Si
 * rowspan=2 style="text-align:right" | 14
 * rowspan=2 style="text-align:right" | 10
 * rowspan=2|24.011535(21)
 * rowspan=2|143.2 (21) ms
 * β+ (65.5%)
 * 24Al
 * rowspan=2|0+
 * rowspan=2|
 * rowspan=2|
 * β+, p (34.5%)
 * 23Mg
 * rowspan=2|25Si
 * rowspan=2 style="text-align:right" | 14
 * rowspan=2 style="text-align:right" | 11
 * rowspan=2|25.004109(11)
 * rowspan=2|220.6(10) ms
 * β+ (65%)
 * 25Al
 * rowspan=2|5/2+
 * rowspan=2|
 * rowspan=2|
 * β+, p (35%)
 * 24Mg
 * 26Si
 * style="text-align:right" | 14
 * style="text-align:right" | 12
 * 25.99233382(12)
 * 2.2453(7) s
 * β+
 * 26Al
 * 0+
 * 27Si
 * style="text-align:right" | 14
 * style="text-align:right" | 13
 * 26.98670469(12)
 * 4.117(14) s
 * β+
 * 27Al
 * 5/2+
 * 28Si
 * style="text-align:right" | 14
 * style="text-align:right" | 14
 * 27.97692653442(55)
 * colspan=3 align=center|Stable
 * 0+
 * 0.92223(19)
 * 0.92205–0.92241
 * 29Si
 * style="text-align:right" | 14
 * style="text-align:right" | 15
 * 28.97649466434(60)
 * colspan=3 align=center|Stable
 * 1/2+
 * 0.04685(8)
 * 0.04678–0.04692
 * 30Si
 * style="text-align:right" | 14
 * style="text-align:right" | 16
 * 29.973770137(23)
 * colspan=3 align=center|Stable
 * 0+
 * 0.03092(11)
 * 0.03082–0.03102
 * 31Si
 * style="text-align:right" | 14
 * style="text-align:right" | 17
 * 30.975363196(46)
 * 157.16(20) min
 * β−
 * 31P
 * 3/2+
 * 32Si
 * style="text-align:right" | 14
 * style="text-align:right" | 18
 * 31.97415154(32)
 * 157(7) y
 * β−
 * 32P
 * 0+
 * trace
 * cosmogenic
 * 33Si
 * style="text-align:right" | 14
 * style="text-align:right" | 19
 * 32.97797696(75)
 * 6.18(18) s
 * β−
 * 33P
 * 3/2+
 * 34Si
 * style="text-align:right" | 14
 * style="text-align:right" | 20
 * 33.97853805(86)
 * 2.77(20) s
 * β−
 * 34P
 * 0+
 * style="text-indent:1em" |34mSi
 * colspan=3 style="text-indent:2em" | 4256.1(4) keV
 * <210 ns
 * IT
 * 34Si
 * (3−)
 * rowspan=2|35Si
 * rowspan=2 style="text-align:right" | 14
 * rowspan=2 style="text-align:right" | 21
 * rowspan=2|34.984550(38)
 * rowspan=2|780(120) ms
 * β−
 * 35P
 * rowspan=2|7/2−#
 * rowspan=2|
 * rowspan=2|
 * β−, n?
 * 34P
 * rowspan=2|36Si
 * rowspan=2 style="text-align:right" | 14
 * rowspan=2 style="text-align:right" | 22
 * rowspan=2|35.986649(77)
 * rowspan=2|503(2) ms
 * β− (88%)
 * 36P
 * rowspan=2|0+
 * rowspan=2|
 * rowspan=2|
 * β−, n (12%)
 * 35P
 * rowspan=3|37Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 23
 * rowspan=3|36.99295(12)
 * rowspan=3|141.0(35) ms
 * β− (83%)
 * 37P
 * rowspan=3|(5/2−)
 * rowspan=3|
 * rowspan=3|
 * β−, n (17%)
 * 36P
 * β−, 2n?
 * 35P
 * rowspan=2|38Si
 * rowspan=2 style="text-align:right" | 14
 * rowspan=2 style="text-align:right" | 24
 * rowspan=2|37.99552(11)
 * rowspan=2|63(8) ms
 * β− (75%)
 * 38P
 * rowspan=2|0+
 * rowspan=2|
 * rowspan=2|
 * β−, n (25%)
 * 37P
 * rowspan=3|39Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 25
 * rowspan=3|39.00249(15)
 * rowspan=3|41.2(41) ms
 * β− (67%)
 * 39P
 * rowspan=3|(5/2−)
 * rowspan=3|
 * rowspan=3|
 * β−, n (33%)
 * 38P
 * β−, 2n?
 * 37P
 * rowspan=3|40Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 26
 * rowspan=3|40.00608(13)
 * rowspan=3|31.2(26) ms
 * β− (62%)
 * 40P
 * rowspan=3|0+
 * rowspan=3|
 * rowspan=3|
 * β−, n (38%)
 * 39P
 * β−, 2n?
 * 38P
 * rowspan=3|41Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 27
 * rowspan=3|41.01417(32)#
 * rowspan=3|20.0(25) ms
 * β−, n (>55%)
 * 40P
 * rowspan=3|7/2−#
 * rowspan=3|
 * rowspan=3|
 * β− (<45%)
 * 41P
 * β−, 2n?
 * 39P
 * rowspan=3|42Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 28
 * rowspan=3|42.01808(32)#
 * rowspan=3|15.5(4 (stat), 16 (sys)) ms
 * β− (51%)
 * 42P
 * rowspan=3|0+
 * rowspan=3|
 * rowspan=3|
 * β−, n (48%)
 * 41P
 * β−, 2n (1%)
 * 40P
 * rowspan=3|43Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 29
 * rowspan=3|43.02612(43)#
 * rowspan=3|13(4 (stat), 2 (sys)) ms
 * β−, n (52%)
 * 42P
 * rowspan=3|3/2−#
 * rowspan=3|
 * rowspan=3|
 * β− (27%)
 * 43P
 * β−, 2n (21%)
 * 41P
 * rowspan=3|44Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 30
 * rowspan=3|44.03147(54)#
 * rowspan=3|4# ms [>360 ns]
 * β−?
 * 44P
 * rowspan=3|0+
 * rowspan=3|
 * rowspan=3|
 * β−, n?
 * 43P
 * β−, 2n?
 * 42P
 * rowspan=3|
 * rowspan=3|
 * β− (<45%)
 * 41P
 * β−, 2n?
 * 39P
 * rowspan=3|42Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 28
 * rowspan=3|42.01808(32)#
 * rowspan=3|15.5(4 (stat), 16 (sys)) ms
 * β− (51%)
 * 42P
 * rowspan=3|0+
 * rowspan=3|
 * rowspan=3|
 * β−, n (48%)
 * 41P
 * β−, 2n (1%)
 * 40P
 * rowspan=3|43Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 29
 * rowspan=3|43.02612(43)#
 * rowspan=3|13(4 (stat), 2 (sys)) ms
 * β−, n (52%)
 * 42P
 * rowspan=3|3/2−#
 * rowspan=3|
 * rowspan=3|
 * β− (27%)
 * 43P
 * β−, 2n (21%)
 * 41P
 * rowspan=3|44Si
 * rowspan=3 style="text-align:right" | 14
 * rowspan=3 style="text-align:right" | 30
 * rowspan=3|44.03147(54)#
 * rowspan=3|4# ms [>360 ns]
 * β−?
 * 44P
 * rowspan=3|0+
 * rowspan=3|
 * rowspan=3|
 * β−, n?
 * 43P
 * β−, 2n?
 * 42P
 * β−?
 * 44P
 * rowspan=3|0+
 * rowspan=3|
 * rowspan=3|
 * β−, n?
 * 43P
 * β−, 2n?
 * 42P
 * β−, 2n?
 * 42P

Silicon-28
Silicon-28, the most abundant isotope of silicon, is of particular interest in the construction of quantum computers when highly enriched, as the presence of 29Si in a sample of silicon contributes to quantum decoherence. Extremely pure (>99.9998%) samples of 28Si can be produced through selective ionization and deposition of 28Si from silane gas. Due to the extremely high purity that can be obtained in this manner, the Avogadro project sought to develop a new definition of the kilogram by making a 93.75 mm sphere of the isotope and determing the exact number of atoms in the sample.

Silicon-28 is produced in stars during the alpha process and the oxygen-burning process, and drives the silicon-burning process in massive stars shortly before they go supernova.

Silicon-29
Silicon-29 is of note as the only stable silicon isotope with a nuclear spin (I = 1/2). As such, it can be employed in nuclear magnetic resonance and hyperfine transition studies, for example to study the properties of the so-called A-center defect in pure silicon.

Silicon-34
Silicon-34 is a radioactive isotope wth a half-life of 2.8 seconds. In addition to the usual N = 20 closed shell, the nucleus also shows a strong Z = 14 shell closure, making it behave like a doubly magic spherical nucleus, except that it is also located two protons above an island of inversion. Silicon-34 has an unusual "bubble" structure where the proton distribution is less dense at the center than near the surface, as the 2s1/2 proton orbital is almost unoccupied in the ground state, unlike in 36S where it is almost full. Silicon-34 is one of the known cluster decay emission particles; it is produced in the decay of 242Cm with a branching ratio of approximately $0$.