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024 7 _ |a 10.1103/PhysRevD.85.014509
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|a Astronomy & Astrophysics
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|a Physics, Particles & Fields
100 1 _ |0 P:(DE-Juel1)132580
|a Dürr, S.
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|u FZJ
245 _ _ |a Sigma term and strangeness content of octet baryons
260 _ _ |a [S.l.]
|b Soc.
|c 2012
264 _ 1 |3 online
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|b American Physical Society (APS)
|c 2012-01-26
264 _ 1 |3 print
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|b American Physical Society (APS)
|c 2012-01-01
300 _ _ |a 014509
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|a Physical Review D
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500 _ _ |a Computations were performed using HPC resources from F.Z. Julich and from GENCI-[IDRIS/ CCRT] (Grant No. 52275) and clusters at Wuppertal and CPT. This work is supported in part by EU Grants No. I3HP, FP7/2007-2013/ERC, No. 208740, No. MRTN-CT-2006-035482 (FLAVIAnet), DFG Grants No. FO 502/2, SFB-TR 55, by CNRS Grant GDR No. 2921, and PICS No. 4707. The authors also thank Martin Jung for pointing out an error in the normalization of the dimensionless sigma terms.
520 _ _ |a By using lattice QCD computations we determine the sigma terms and strangeness content of all octet baryons by means of an application of the Hellmann-Feynman theorem. In addition to polynomial and rational expressions for the quark-mass dependence of octet members, we use SU(3) covariant baryon chiral perturbation theory to perform the extrapolation to the physical up and down quark masses. Our Nf = 2 + 1 lattice ensembles include pion masses down to about 190 MeV in large volumes (M pi L greater than or similar to 4), and three values of the lattice spacing. Our main results are the nucleon sigma term sigma(pi N) = 39(4)((+18)(-7)) and the strangeness content y(N) = 0.20(7)((+13)(-17)). Under the assumption of validity of covariant baryon chi PT in our range of masses one finds y(N) = 0.276(77)((+90)(-62)).
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