  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.
