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Explores volume effects on baryon masses in light hadrons, suggesting insights for future studies.
The volume dependence of the octet baryon masses and relations among them are explored with Lattice QCD. Calculations are performed with nf=2+1 clover fermion discretization in four lattice volumes, with spatial extent L~2.0, 2.5, 3.0 and 3.9 fm, with an anisotropic lattice spacing of bₛ~0.123 fm in the spatial direction, and bₜ=bₛ/3.5 in the time direction, and at a pion mass of m_π~390 MeV. The typical precision of the ground-state baryon mass determination is 0.2%, enabling a precise exploration of the volume dependence of the masses, the Gell-Mann--Okubo mass relation, and of other mass combinations. A comparison of the volume dependence with the predictions of heavy baryon chiral perturbation theory is performed in both the SU(2)LSU(2)R and SU(3)LSU(3)R expansions. Predictions of the three-flavor expansion for the hadron masses are found to describe the observed volume dependences reasonably well. Further, the ΔNπ axial coupling constant is extracted from the volume dependence of the nucleon mass in the two-flavor expansion, with only small modifications in the three-flavor expansion from the inclusion of kaons and η's. At a given value of m_πL, the finite-volume contributions to the nucleon mass are predicted to be significantly smaller at m_π~140 MeV than at m_π~390 MeV due to a coefficient that scales as ~m_π³. This is relevant for the design of future ensembles of lattice gauge-field configurations. Finally, the volume dependence of the pion and kaon masses are analyzed with two-flavor and three-flavor chiral perturbation theory.
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Beane et al. (2011) studied this question.
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