Non-perturbative RG for the Weak interaction corrections to the magnetic moment

We analyze, by rigorous Renormalization Group (RG) methods, a Fermi model for Weak forces with a single family of leptons, one massless and the other with mass $m=M e^{-\beta}$, with $M$ the gauge boson mass, a quartic non-local interaction with coupling $\lambda^2$ and a momentum cut-off $\Lambda$. The magnetic moment is written as a series in $\lambda^2$, with $n$-th coefficients bounded by $C^n ({m^2\over M^2}) \beta^{2n } ({\Lambda^2\over M^2})^{(1+0^+)(n-1)}$ if $C$ a constant; this implies convergence and provides non-perturbative bounds on the higher orders contribution. The fact that the magnetic moment is associated to a dimensionally irrelevant quantity requires the implementation of cancellations in the multiscale analysis.