Charge-Exchange and Double Beta Decay
In beta decay, an unstable nucleus decays to a nucleus containing (Z+1) or (Z-1) protons and an identical
mass number. However, beta decay proceeds towards the valley of stability (a region of stable nuclei), and if scientists want to explore
charge-exchange reactions in the opposite direction (away from stability), a hadronic probe is often used.
Some nuclear beta transitions are "forbidden" decays because of angular momentum selection rules. In addition, because of the
limited energy available for the decay, single beta decay is only possible to a limited number of final states. In select
cases, a combination of 2 beta decays (Z to Z+2) becomes the only possible mode of decay.
Double beta decay is so rare that
parent isotopes are often described as "stable," and half lives run around 1020 years. Two-neutrino double beta
decay has been observed. Neutrinoless double beta decay (0νββ) has not yet been observed conclusively. Such an observation
would be groundbreaking and exciting, because the existence of this type of decay would tell physicists much about the nature
of the neutrino.
The half life for 0νββ decay depends on matrix elements that can only be calculated in theory. However,
the calculation of such matrix elements can be constrained by data obtained via charge-exchange experiments on targets made of
the initial and final nuclei involved in 0νββ decay. In such experiments, excited states in the intermediate
nucleus (Z+1) are populated.
We have planned two charge-exchange experiments to measure such transitions: a (t,3He)
experiment on the Z+2 nucleus at the NSCL and a (3He,t) experiment on the Z nucleus at RCNP. Each reaction
will produce excited states in the Z+1 nucleus, and the results should provide a comprehensive picture of the transition
strengths and allow us to constrain the calculations of 0νββ matrix elements.