2026-07-072026-07-07http://salesiana.dossiersoluciones.com/handle/123456789/39185We evaluate the axial anomaly for the general Ginsparg-Wilson fermion operator $D = D_c (\Id + R D_c)^{-1}$ with $R = r \Id$. For any chirally symmetric $D_c$ which in the free fermion limit, is free of species doubling and behaves like $i γ_μp_μ$ as $p \to 0$, the axial anomaly $\tr[γ_5 (R D) (x,x)]$ for U(1) lattice gauge theory with single fermion flavor is equal to $e^2/(32 π^2) ε_{μνλσ} F_{μν}(x) F_{λσ}(x+\hatμ+\hatν)$ plus terms which are higher orders and/or non-perturbative contribtuons. The $F \tilde{F}$ term is r-invariant and has the correct continuum limit.38 pages, latex, 1 figure, add appendix C and several remarksHigh Energy Physics - LatticeHigh Energy Physics - PhenomenologyHigh Energy Physics - TheoryPerturbation calculation of the axial anomaly of Ginsparg-Wilson fermiontext