Perturbation calculation of the axial anomaly of Ginsparg-Wilson fermion

Abstract

We 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 $i{\gamma }_{\mu }{p}_{\mu }$ 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 $e^2/(32{\pi }^2){\epsilon }_{\mu \nu \lambda \sigma }{F}_{\mu \nu }(x)F_{\lambda \sigma }(x+\hat{\mu }+\hat{\nu })$ 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.

arXiv comment38 pages, latex, 1 figure, add appendix C and several remarks

References in corpus (4)

• Topology and the axial anomaly in abelian lattice gauge theories
• GW fermion propagators and chiral condensate
• The theoretical background and properties of perfect actions
• Topological Phases in Neuberger-Dirac operator

Cited by in corpus (10)

• Weyl fermions on the lattice and the non-abelian gauge anomaly
• Axial anomaly with the overlap-Dirac operator in arbitrary dimensions
• The index of the overlap Dirac operator on a discretized 2d non-commutative torus
• Topological Phases in Neuberger-Dirac operator
• More about the axial anomaly on the lattice
• A construction of chiral fermion action
• A lattice implementation of the eta-invariant and effective action for chiral fermions on the lattice
• Wess-Zumino-Witten term on the lattice
• Fermion determinant and chiral anomaly on a finite lattice
• Chiral fermions on a finite lattice