Low-Energy Constants of Chiral Perturbation Theory from Pion Scalar Form Factors in N_{f}=2+1-Flavor Lattice QCD with Controlled Errors
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Updated: Jan 18, 2026

Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
Georg von Hippel1, Konstantin Ottnad1
1Johannes Gutenberg-Universität Mainz, PRISMA, +, Cluster of Excellence and Institut für Kernphysik, 55099 Mainz, Germany.
Abstract:
We determine the low-energy constants f_{0}, L_{4}^{r} and L_{5}^{r} of SU(3) chiral perturbation theory from a lattice QCD calculation of the scalar form factors of the pion with fully controlled systematics. Lattice results are computed on a large set of N_{f}=2+1 gauge ensembles covering four lattice spacings a∈[0.049,0.086] fm, pion masses M_{π}∈[130,350] MeV, and various large physical volumes. By determining the notorious quark-disconnected contributions with unprecedented precision and using a large range of source-sink separations t_{sep}∈[1.0,3.25] fm, we are able for the first time to obtain the scalar radii from a z-expansion parametrization of the form factors rather than a simple linear approximation at small momentum transfer. The low-energy constants are obtained from the physical extrapolation of the radii using next-to-leading-order SU(3) next-to-leading-order chiral perturbation theory to parametrize the quark mass dependence. Systematic uncertainties are estimated via model averages based on the Akaike information criterion. Our determination of L_{4}^{r} is the first lattice determination to obtain a result not compatible with zero.
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