The beta decay is caused by the weak interaction. The weak interaction is very short range, because the mediate particles, the and bosons are 80 GeV and 91 GeV respectively. The effective range is like fm. So, the interaction can assumed to be a delta function and only the coupling constant matter. The Fermi coupling constant is .

The fundamental process of beta decay is the decay of quark.

Since a pion is made from up and down quark, the decay of pion into position and electron neutrino is also due to weak interaction.

The Hamilton of the beta decay is

where is the vector coupling constant, the term is called Fermi transition. The is the isospin ladder operator. The beta+ decay changes the isospin from +1/2 (neutron) to -1/2 (proton). The is the axial coupling constant, the term is called Gamow-Teller transition. is spin operator. Because of this operator, the Gamow-Teller transition did not preserve parity.

The is different from is caused by the effect of strong interaction. The Goldberger-Trieman relation

where is the pion decay constant. is the coupling constant between pion and nucleon. This, we can see the effect of the strong interaction, in which pion is the meson for strong nuclear force.

The transition probability can be estimated by Fermi-Golden rule

the final state wavefunction

using long wavelength approximation, the spherical Bessel function can be approximated by the first term.

The first term 1, or L=0 is called allowed decay, so that the orbital angular momentum of the decayed nucleus unchanged. The higher order term, in which the weak interaction have longer range has very small probability and called L-th forbidden decay.

The density of state is

where the is the Fermi function.

The total transition probability is the integration with respect to the electron momentum.

where is the Fermi integral. The half-life

To focus on the beta decay from the interference of the density of state, the ft-value is

The ft-value could be difference by several order.

There is a super-allowed decay from with same isospin, which the GT does not involve. an example is

14O 14N

The ft-value is 3037.7s, the smallest of known.

Fermi | Gamow-Teller |
---|---|

transition | L | |||||
---|---|---|---|---|---|---|

Fermi | GT | |||||

Super allowed | 3.1 ~ 3.6 | not exist | 0 | no | ||

allowed | 0 | 2.9 ~ 10 | 0 | (0), 1 | 0, 1 ; forbidden | no |

1st forbidden | 1 | 5 ~ 19 | (0),1 | 0, 1, 2 | 0,1 | yes |

2nd forbidden | 2 | 10 ~18 | (1), 2 | 2, 3 | no | |

3rd forbidden | 3 | 17 ~ 22 | (2), 3 | 3, 4 | yes | |

4th forbidden | 4 | 22 ~ 24 | (3), 4 | 4, 5 | no |

The () means not possible if either initial or final state is zero. i.e is not possible for 1st forbidden.