2007
DOI: 10.1103/physrevd.75.073015
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Hadron spectrum, quark masses, and decay constants from light overlap fermions on large lattices

Abstract: We present results from a simulation of quenched overlap fermions with Lüscher-Weisz gauge field action on lattices up to 24 3 48 and for pion masses down to ≈ 250 MeV. Among the quantities we study are the pion, rho and nucleon masses, the light and strange quark masses, and the pion decay constant. The renormalization of the scalar and axial vector currents is done nonperturbatively in the RI − M OM scheme. The simulations are performed at two different lattice spacings, a ≈ 0.1 fm and ≈ 0.15 fm, and on two … Show more

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Cited by 19 publications
(14 citation statements)
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References 63 publications
(59 reference statements)
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“…We measure the history of the topological charge Q to monitor the possible emergence of topological freezing, which might affect spectral measurements [89,90] (see also Refs. [91,92]).…”
Section: Scale Setting and Topologymentioning
confidence: 99%
“…We measure the history of the topological charge Q to monitor the possible emergence of topological freezing, which might affect spectral measurements [89,90] (see also Refs. [91,92]).…”
Section: Scale Setting and Topologymentioning
confidence: 99%
“…[69]). Secondly, the values of physical observables depend on which topological sector a configuration is in [70]; sampling a single Q or an unrepresentative distribution of Qs will introduce an uncontrolled systematic error. It is therefore necessary to verify that Q not only moves sufficiently rapidly, but also displays the expected Gaussian histogram.…”
Section: Topological Charge Historymentioning
confidence: 99%
“…In more detail, we carry out the numerical computations by the technique of Refs. [20][21][22]. The massless overlap Dirac operator D(p) is save 0(80) pairs of the low-lying eigenvalues and eigen vectors of the overlap Dirac operator.…”
Section: B Simulation Detailsmentioning
confidence: 99%
“…In any case, as a dual superconductor the vacuum shields the monop oles, so that they are one-dimensional structures and do not influence the external space time: 0(V~i). For these reasons we expect that the distribution of zero modes (19)- (20) is unaffected by the additional monopoles espe cially at large space-time volumes V, except for the addition of some instantons.…”
Section: A Simulation Detailsmentioning
confidence: 99%