Role of the $σ$-resonance in determining the convergence of chiral perturbation theory
| dc.creator | Cecile, D. J. | |
| dc.creator | Chandrasekharan, Shailesh | |
| dc.date | 2008-01-24 | |
| dc.date.accessioned | 2026-07-07T11:55:32Z | |
| dc.date.available | 2026-07-07T11:55:32Z | |
| dc.description | The dimensionless parameter $ξ= M_π^2/(16 π^2 F_π^2)$, where $F_π$ is the pion decay constant and $M_π$ is the pion 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 $p$-regime and the $ε$-regime as expected. However, $ξ\lesssim 0.002$ is necessary before 1-loop chiral perturbation theory predicts the data within 1%. For $ξ> 0.0035$ the data begin to deviate dramatically 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.description | 5 pages, 6 figures, revtex format | |
| dc.identifier | https://arxiv.org/abs/0801.3823 | |
| dc.identifier | http://arxiv.org/abs/0801.3823 | |
| dc.identifier | Phys.Rev.D77:091501,2008 | |
| dc.identifier | doi:10.1103/PhysRevD.77.091501 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/205276 | |
| dc.subject | High Energy Physics - Lattice | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | Nuclear Theory | |
| dc.title | Role of the $σ$-resonance in determining the convergence of chiral perturbation theory | |
| dc.type | text |