Positron emission

Nuclear physics
Nucleus · Nucleons (p, n) · Nuclear force · Nuclear reaction
Nuclear models and stability Liquid drop · Nuclear shell · Nuclear structure Binding energy · p–n ratio · Drip line · Stability Isl.
Nuclides' classification Isotopes – equal Z Isobars – equal A Isotones – equal N Isodiaphers – equal N − Z      Isomers – equal all the above Mirror nuclei – Z ↔ N Stable · Magic · Even/odd · Halo
Radioactive decay Alpha α · Beta β (2β, β+) · K/L capture · Isomeric (Gamma γ · Internal conversion) · Spontaneous fission · Cluster decay · Neutron emission · Proton emission Decay energy · Decay chain · Decay product · Radiogenic nuclide
Nuclear fission Spontaneous · Products (pair breaking) · Photofission
Capturing processes electron · neutron (s · r) · proton (p · rp)
High energy processes Spallation (by cosmic ray) · Photodisintegration
Nucleosynthesis topics Nuclear fusion Processes: Stellar · Big Bang · Supernova Nuclides: Primordial · Cosmogenic · Artificial
Scientists Becquerel · Davisson · Bethe · Skłodowska-Curie · Pi.Curie · Fr.Curie · Ir.Curie · Fermi · Oppenheimer · Rutherford · Thomson  · Chadwick · Oliphant · Szilárd  · Teller · Lawrence · Proca · Mayer · Jensen · Alvarez · Soddy · Rabi · Meitner · Strassmann · Hahn · Purcell · Walton · Cockcroft ·
v t e

Positron emission or beta plus decay (β⁺ decay) is a particular type of radioactive decay and a subtype of beta decay, in which a proton inside a radionuclide nucleus is converted into a neutron while releasing a positron and an electron neutrino (ν_e).^[1] Positron emission is mediated by the weak force. The positron is a type of beta particle (β⁺), the other beta particle being the electron (β^-) emitted from the β^{- decay of a nucleus.}

An example of positron emission (β⁺ decay) is shown with magnesium-23 decaying into sodium-23:

23
12Mg → 23
11Na + e+ + ν
e

Because positron emission decreases proton number relative to neutron number, positron decay happens typically in large "proton-rich" radionuclides. Positron decay results in nuclear transmutation, changing an atom of a chemical element into an atom of an element with an atomic number that is less by one unit.

Positron emission should not be confused with electron emission or beta minus decay (β^- decay), which occurs when a neutron turns into a proton and the nucleus emits an electron and an antineutrino. Electron capture (sometimes called inverse beta decay) is also occasionally classified as a type of beta decay. (In some ways, electron capture can be regarded as the "opposite" of positron emission. It can only occur when electrons are available and requires less energy difference between parent and daughter, so occurs much more often in smaller atoms than positron emission does.)

Discovery of positron emission

In 1934 Frédéric and Irène Joliot-Curie bombarded aluminium with alpha particles to effect the nuclear reaction 4
2He + 27
13Al → 30
15P + 1
0n, and observed that the product isotope 30
15P emits a positron identical to those found in cosmic rays by Carl David Anderson in 1932. This was the first example of β+ decay (positron emission). The Curies termed the phenomenon "artificial radioactivity," since 30
15P is a short-lived nuclide which does not exist in nature. The discovery of artificial radioactivity would be cited when the husband and wife team won the Nobel Prize.

Positron-emitting isotopes

Isotopes which undergo this decay and thereby emit positrons include carbon-11, potassium-40, nitrogen-13, oxygen-15, aluminium-26, sodium-22, fluorine-18, and iodine-121. As an example, the following equation describes the beta plus decay of carbon-11 to boron-11, emitting a positron and a neutrino:

11 6C

→

11 5B

+

e+

+

ν e

+

0.96 MeV

Emission mechanism

Inside protons and neutrons, there are fundamental particles called quarks. The two most common types of quarks are up quarks, which have a charge of +²/₃ and down quarks, with a −¹/₃ charge. Quarks arrange themselves in sets of three such that they make protons and neutrons. In a proton, whose charge is +1, there are two up quarks and one down quark. Neutrons, with no charge, have one up quark and two down quarks. Via the weak interaction, quarks can change flavor from down to up, resulting in electron emission. Positron emission happens when an up quark changes into a down quark.^[2]

Nuclei which decay by positron emission may also decay by electron capture. For low-energy decays, electron capture is energetically favored by 2m_ec² = 1.022 MeV, since the final state has an electron removed rather than a positron added. As the energy of the decay goes up, so does the branching ratio towards positron emission. However, if the energy difference is less than 2m_ec², then positron emission cannot occur and electron capture is the sole decay mode. Certain isotopes (for instance, 7Be) are stable in galactic cosmic rays, because the electrons are stripped away and the decay energy is too small for positron emission.

Application

These isotopes are used in positron emission tomography, a technique used for medical imaging. Note that the energy emitted depends on the isotope that is decaying; the figure of 0.96 MeV applies only to the decay of carbon-11. Isotopes which increase in mass under the conversion of a proton to a neutron, or which decrease in mass by less than 2m_e, cannot spontaneously decay by positron emission.

The short-lived positron emitting isotopes ¹¹C, ¹³N, ¹⁵O and ¹⁸F used for positron emission tomography are typically produced by proton irradiation of natural or enriched targets.^[3][4]

References

External links

• The LIVEChart of Nuclides - IAEA with filter on β⁺ decay