Abstract
Following Allen's comments, the authors discuss and clarify here some points of their theoretical calculation of electron-phonon effects in lead. It is numerically demonstrated that the low-energy part of α2F(ω) does not significantly contribute to m*(T) in the experimental T, ω domain. Moreover, using a calculation averaged more correctly, the authors obtain a good agreement with their experimental results when comparing T and ω effects on m*(T,ω).