1999
DOI: 10.1016/s0370-2693(99)00021-0
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Weak coupling expansion of massless QCD with a Ginsparg-Wilson fermion and axial U(1) anomaly

Abstract: We discuss the weak coupling expansion of massless QCD with the Dirac operator which is derived by Neuberger based on the overlap formalism and satisfies the Ginsparg-Wilson relation. The axial U(1) anomaly associated to the chiral transformation proposed by Lüscher is calculated as an application and is shown to have the correct form of the topological charge density for perturbative backgrounds. The coefficient of the anomaly is evaluated as a winding number related to a certain five-dimensional fermion prop… Show more

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Cited by 127 publications
(166 citation statements)
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“…This is directly related to the connection with the index theorems in the continuum; for recent reviews see Adams (2000) and Kerler (2000). Recent detailed analysis (Luscher, 2000;Kikukawa and Yamada, 1999) shows that this operator is particularly well behaved order by order in perturbation theory. This has led to hopes that this may lead the way to a rigorous formulation of chiral models, such as the standard model.…”
Section: The Ginsparg-wilson Relationmentioning
confidence: 87%
“…This is directly related to the connection with the index theorems in the continuum; for recent reviews see Adams (2000) and Kerler (2000). Recent detailed analysis (Luscher, 2000;Kikukawa and Yamada, 1999) shows that this operator is particularly well behaved order by order in perturbation theory. This has led to hopes that this may lead the way to a rigorous formulation of chiral models, such as the standard model.…”
Section: The Ginsparg-wilson Relationmentioning
confidence: 87%
“…It can be seen, for example, from the computation of chiral anomaly [38,39]. In what follows, r is fixed to the standard value r = 1.…”
Section: Lattice Formulations With Overlap Dirac Operatormentioning
confidence: 99%
“…Tr(γ 3 a D) has been computed in the two-dimensional case [38], assuming that A µ (x) appearing in the expansion of U µ (x) = e iaAµ(x) are smooth external variables. We obtain…”
Section: Q-supersymmetry Transformationmentioning
confidence: 99%
“…where γ is a constant independent of the gauge fields, which takes the value γ = 1 32π 2 for the overlap Dirac operator [78], β µν (x) is a tensor field satisfying ∂ * µ β µν (x) = 0 which depends only on the SU(2) gauge field and k µ (x) is a local, gauge-invariant current which can be constructed so that it transforms as the axial vector current under the lattice symmetries. Moreover, taking into account the pseudo-scalar nature of q (1) L (x) under the charge conjugation and the pseudo reality of SU (2), one has…”
Section: Cancellations Of Sumentioning
confidence: 99%