Sigma-resonance and convergence of chiral perturbation theory

dc.creatorCecile, D. J.
dc.creatorChandrasekharan, Shailesh
dc.date2008-10-14
dc.date.accessioned2026-07-07T12:39:45Z
dc.date.available2026-07-07T12:39:45Z
dc.descriptionThe dimensionless parameter $ξ' = M^2/(16 π^2 F^2)$, where $F$ is the pion decay constant in the chiral limit and $M$ is the pion mass at leading order in the quark mass, is expected to control the convergence of chiral perturbation theory applicable to QCD. Here we demonstrate that a strongly coupled lattice gauge theory model with the same symmetries as two-flavor QCD but with a much lighter $σ$-resonance is different. Our model allows us to study efficiently the convergence of chiral perturbation theory as a function of $ξ'$. We first confirm that the leading low energy constants appearing in the chiral Lagrangian are the same when calculated from the $ε$-regime and the $p$-regime. However, $ξ' \lesssim 0.002$ is necessary before 1-loop chiral perturbation theory predicts the data within 1%. However, for $ξ' > 0.0035$ the data begin to deviate qualitatively from 1-loop chiral perturbation theory predictions. We argue that this qualitative change is due to the presence of a light $σ$-resonance in our model. Our findings may be useful for lattice QCD studies.
dc.description7 pages, 9 figures;talk presented at the XXVI International Symposium on Lattice Field Theory, July 14 - 19, 2008, Williamsburg, Virginia, USA
dc.identifierhttps://arxiv.org/abs/0810.2423
dc.identifierhttp://arxiv.org/abs/0810.2423
dc.identifierPoS LATTICE2008:071,2008
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/219224
dc.subjectHigh Energy Physics - Lattice
dc.titleSigma-resonance and convergence of chiral perturbation theory
dc.typetext

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