Abstract

We determine the NLO chiral low-energy constant L10rL_{10}^r, and combinations C12r±C61r+C80rC_{12}^r\pm C_{61}^r+C_{80}^r, C13r−C62r+C81rC_{13}^r-C_{62}^r+C_{81}^r, C61rC_{61}^r, and C87rC_{87}^r, of the NNLO chiral low-energy constants incorporating recently revised ALEPH results for the non-strange vector (VV) and axial-vector (AA) hadronic ττ decay distributions and recently updated RBC/UKQCD lattice data for the non-strange V−AV-A two-point function. In the MSˉ\bar{\rm MS} scheme, at renormalization scale μ=770 MeVμ=770\ {MeV}, we find L10r=−0.00350(17)L_{10}^r=-0.00350(17), C12r+C61r+C80r=0.00237(16) GeV−2C_{12}^r+C_{61}^r+C_{80}^r=0.00237(16)\ {GeV}^{-2}, C12r−C61r+C80r=−0.00056(15) GeV−2C_{12}^r-C_{61}^r+C_{80}^r=-0.00056(15)\ {GeV}^{-2}, C13r−C62r+C81r=0.00046(9) GeV−2C_{13}^r-C_{62}^r+C_{81}^r=0.00046(9)\ {GeV}^{-2}, C61r=0.00146(15) GeV−2C_{61}^r=0.00146(15)\ {GeV}^{-2}, and C87r=0.00510(22) GeV−2C_{87}^r=0.00510(22)\ {GeV}^{-2}. With errors here at or below the level expected for contributions of yet higher order in the chiral expansion, the analysis exhausts the possibilities of what can be meaningfully achieved in an NNLO analysis. We also consider the dimension six and dimension eight coefficients in the operator product expansion in the V−AV-A channel.

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