Abstract

We determine the relative pion mass shift Mπ(L)/Mπ−1M_π(L)/M_π-1 due to the finite spatial extent LL of the box by means of two-flavor chiral perturbation theory and the one-particle Lüscher formula. We use as input the expression for the infinite volume ππππ forward scattering amplitude up to next-to-next-to-leading order and can therefore control the convergence of the chiral series. A comparison to the full leading order chiral expression for the pion mass in finite volume allows us to check the size of subleading terms in the large-LL expansion.

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