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000185649 0247_ $$2doi$$a10.1103/PhysRevD.90.114504
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000185649 0247_ $$2ISSN$$a1550-7998
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000185649 1001_ $$0P:(DE-Juel1)132580$$aDürr, Stephan$$b0$$eCorresponding Author$$ufzj
000185649 245__ $$aLattice QCD at the physical point meets $SU\left(2\right)$ chiral perturbation theory
000185649 260__ $$a[S.l.]$$bSoc.$$c2014
000185649 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2014-12-16
000185649 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2014-12-01
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000185649 500__ $$aarXiv:1310.3626
000185649 520__ $$aWe perform a detailed, fully correlated study of the chiral behavior of the pion mass and decay constant, based on 2+1 flavor lattice QCD simulations. These calculations are implemented using tree-level, O(a)-improved Wilson fermions, at four values of the lattice spacing down to 0.054 fm and all the way down to below the physical value of the pion mass. They allow a sharp comparison with the predictions of SU(2) chiral perturbation theory (χPT) and a determination of some of its low energy constants. In particular, we systematically explore the range of applicability of next-to-leading order (NLO) SU(2) χPT in two different expansions: the first in quark mass (x expansion), and the second in pion mass (ξ expansion). We find that these expansions begin showing signs of failure for Mπ≳300  MeV, for the typical percent-level precision of our Nf=2+1 lattice results. We further determine the LO low energy constants (LECs), F=88.0±1.3±0.2 and BMS¯(2  GeV)=2.61(6)(1)  GeV, and the related quark condensate, ΣMS¯(2  GeV)=(272±4±1  MeV)3, as well as the NLO ones, ℓ¯3=2.6(5)(3) and ℓ¯4=3.7(4)(2), with fully controlled uncertainties. We also explore the next-to-next-to-leading order (NNLO) expansions and the values of NNLO LECs. In addition, we show that the lattice results favor the presence of chiral logarithms. We further demonstrate how the absence of lattice results with pion masses below 200 MeV can lead to misleading results and conclusions. Our calculations allow a fully controlled, ab initio determination of the pion decay constant with a total 1% error, which is in excellent agreement with experiment.
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000185649 7001_ $$0P:(DE-HGF)0$$aFodor, Zoltán$$b1
000185649 7001_ $$0P:(DE-HGF)0$$aHoelbling, Christian$$b2
000185649 7001_ $$0P:(DE-Juel1)132171$$aKrieg, Stefan$$b3$$ufzj
000185649 7001_ $$0P:(DE-HGF)0$$aKurth, Thorsten$$b4
000185649 7001_ $$0P:(DE-HGF)0$$aLellouch, Laurent$$b5
000185649 7001_ $$0P:(DE-Juel1)132179$$aLippert, Thomas$$b6$$ufzj
000185649 7001_ $$0P:(DE-HGF)0$$aMalak, Rehan$$b7
000185649 7001_ $$0P:(DE-HGF)0$$aMétivet, Thibaut$$b8
000185649 7001_ $$0P:(DE-HGF)0$$aPortelli, Antonin$$b9
000185649 7001_ $$0P:(DE-HGF)0$$aSastre, Alfonso$$b10
000185649 7001_ $$0P:(DE-Juel1)161563$$aSzabó, Kálmán$$b11$$ufzj
000185649 77318 $$2Crossref$$3journal-article$$a10.1103/physrevd.90.114504$$b : American Physical Society (APS), 2014-12-16$$n11$$p114504$$tPhysical Review D$$v90$$x1550-7998$$y2014
000185649 773__ $$0PERI:(DE-600)2844732-3$$a10.1103/PhysRevD.90.114504$$gVol. 90, no. 11, p. 114504$$n11$$p114504$$tPhysical review / D$$v90$$x1550-7998$$y2014
000185649 8564_ $$uhttp://arxiv.org/abs/arXiv:1310.3626
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