Within QRPA we achieve partial restoration of the isospin symmetry and hence fulfillment of the requirement that the $2\nu\beta\beta$ Fermi matrix element $M^{ 2\nu}_F$ vanishes, as it should, unlike in the previous version of the method. This is accomplished by separating the renormalization parameter $g_{ pp}$ of the particle-particle proton-neutron interaction into the isovector and isoscalar parts. The isovector parameter $g_{ pp}^{ T=1}$ need to be chosen to be essentially equal to the pairing constant $g_{ pair}$, so no new parameter is needed. For the $0\nu\beta\beta$ decay the Fermi matrix element $M^{ 0\nu}_F$ is substantially reduced, while the full matrix element $M^{ 0\nu}$ is reduced by $\approx$ 10%. We argue that this more consistent approach should be used from now on in the proton-neutron QRPA and in analogous methods.
Categories: nucl-th hep-ph