Isotopes of helium

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Helium (He)
Standard atomic mass: 4.002602(2) u

Contents

For more details on this topic, see Helium-3.
For more details on this topic, see Helium-4.

Although there are eight known isotopes of helium, only helium-3 and helium-4 are stable. In the Earth's atmosphere, there is one He-3 atom for every million He-4 atoms.[1] However, helium is unusual in that its isotopic abundance varies greatly depending on its origin. In the interstellar medium, the proportion of He-3 is around a hundred times higher.[2] Rocks from the Earth's crust have isotope ratios varying by as much as a factor of ten; this is used in geology to study the origin of such rocks.

The most common isotope, helium-4, is produced on Earth by alpha decay of heavier radioactive elements; the alpha particles that emerge are fully ionized helium-4 nuclei. Helium-4 is an unusually stable nucleus because its nucleons are arranged into complete shells. It was also formed in enormous quantities during Big Bang nucleosynthesis.

Equal mixtures of liquid helium-3 and helium-4 below 0.8 K will separate into two immiscible phases due to their dissimilarity (they follow different quantum statistics: helium-4 atoms are bosons while helium-3 atoms are fermions).[3] Dilution refrigerators take advantage of the immiscibility of these two isotopes to achieve temperatures of a few millikelvins. There is only a trace amount of helium-3 on Earth, primarily present since the formation of the Earth, although some falls to Earth trapped in cosmic dust.[4] Trace amounts are also produced by the beta decay of tritium.[5] In stars, however, helium-3 is more abundant, a product of nuclear fusion. Extraplanetary material, such as lunar and asteroid regolith, have trace amounts of helium-3 from being bombarded by solar winds.

The different formation processes of the two stable isotopes of helium produce the differing isotope abundances. These differing isotope abundances can be used to investigate the origin of rocks and the composition of the Earth's mantle.[4]

A subset of exotic light nuclei, the exotic helium isotopes have larger atomic masses than helium's natural isotopes. Although all exotic helium isotopes decay with a half-life of less than one second, researchers have eagerly created exotic light isotopes through particle accelerator collisions to create unusual atomic nuclei for elements such as helium, lithium, and nitrogen. The bizarre nuclear structures of such isotopes may offer insight into the isolated properties of neutrons.

The shortest-lived isotope is helium-5 with a half-life of 7.6×10−22 second. Helium-6 decays by emitting a beta particle and has a half life of 0.8 second. Helium-7 also emits a beta particle as well as a gamma ray. The most widely-studied exotic helium isotope is helium-8. This isotope is thought to consist of a normal helium-4 nucleus surrounded by four neutrons dubbed a "halo" (6He also has a halo of neutrons). Halo nuclei have become an area of intense research. Isotopes up to helium-10, with two protons and eight neutrons, have been confirmed. Helium-7 and helium-8 are hyperfragments that are created in certain nuclear reactions.[6]

For more details on this topic, see Diproton.

Helium-2 is a hypothetical isotope of Helium which according to theoretical calculations would have existed if the strong force had been 2% greater.

nuclide
symbol
Z(p) N(n) isotopic mass (u) half-life nuclear
spin
representative
isotopic
composition
(mole fraction)
range of natural
variation
(mole fraction)
notes
3He 2 1 3.0160293191(26) STABLE 1/2+ 0.00000134(3) 4.6×10-10-0.000041
4He 2 2 4.00260325415(6) STABLE 0+ 0.99999866(3) 0.999959-1
5He 2 3 5.01222(5) 700(30)E-24 s [0.60(2) MeV] 3/2-
Highly unstable, decays to 4He.
6He 2 4 6.0188891(8) 806.7(15) ms 0+
Produced from 7He or 11Li, decomposes to 6Li through beta decay (beta-minus).
7He 2 5 7.028021(18) 2.9(5)E-21 s [159(28) keV] (3/2)-
Highly unstable, decays to 6He.
8He 2 6 8.033922(7) 119.0(15) ms 0+
Produced from 9He, decomposes to 7Li through beta decay then emits a delayed neutron.
9He 2 7 9.04395(3) 7(4)E-21 s [100(60) keV] 1/2(-#)
Highly unstable, decays to 8He.
10He 2 8 10.05240(8) 2.7(18)E-21 s [0.17(11) MeV] 0+
Highly unstable, decays to 9He.

  • The isotopic composition refers to that in air.
  • The precision of the isotope abundances and atomic mass is limited through variations. The given ranges should be applicable to any normal terrestrial material.
  • Geologically exceptional samples are known in which the isotopic composition lies outside the reported range. The uncertainty in the atomic mass may exceed the stated value for such specimens.
  • 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 expanded uncertainties.

  1. ^ Emsley, John. Nature's Building Blocks: An A-Z Guide to the Elements. Oxford: Oxford University Press, 2001. Page 178. ISBN 0-19-850340-7
  2. ^ [1], ingentaconnect.com, Retrieved 5 January 2007
  3. ^ The Encyclopedia of the Chemical Elements, page 264
  4. ^ a b http://www.mantleplumes.org/HeliumFundamentals.html
  5. ^ http://environmentalchemistry.com/yogi/periodic/Li-pg2.html
  6. ^ The Encyclopedia of the Chemical Elements, page 260

  • General Tables — abstracts for helium and other exotic light nuclei


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