Abstract
A cutoff-dependent formulation of renormalized perturbation theory is used to study the Gaussian-to-Heisenberg crossover, describing the changeover from tricritical to critical-line behavior, for the specific heat, to second order in ε=4d, in extension of earlier work by Bruce and Wallace for the susceptibility. The role of the nonhomogeneous part of the renormalization-group equation for the bare vertex function Γ(2,0) - proportional to the specific heat - with two φ2 insertions is discussed in detail in an isotropic φ4 field model. An explicit crossover scaling function for the specific heat is calculated and the effective exponent αeff is found to differ considerably from an earlier first-order calculation.