by a single renormalized Anderson model, with three parameters, an effective level
̃\epsilon_d, an effective hybridization ̃V, and a quasiparticle interaction ̃U. The renormalized
parameters are calculated as a function of the bare parameters for a number of impurity
models, including those with coupling to phonons and a Falikov-Kimball interaction term. In
the model with a coupling to phonons we determine where the interaction of the …