Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/76479
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dc.contributor.authorHorsley, R.-
dc.contributor.authorNakamura, Y.-
dc.contributor.authorPerlt, H.-
dc.contributor.authorPleiter, D.-
dc.contributor.authorRakow, P.-
dc.contributor.authorSchierholz, G.-
dc.contributor.authorSchiller, A.-
dc.contributor.authorStüben, H.-
dc.contributor.authorWinter, F.-
dc.contributor.authorZanotti, J.-
dc.date.issued2012-
dc.identifier.citationPhysical Review D: Particles, Fields, Gravitation and Cosmology, 2012; 85(3):034506:1-034506:12-
dc.identifier.issn1550-7998-
dc.identifier.issn1550-2368-
dc.identifier.urihttp://hdl.handle.net/2440/76479-
dc.description.abstractQCD lattice simulations determine hadron masses as functions of the quark masses. From the gradients of these masses and using the Feynman-Hellmann theorem the hadron sigma terms can then be determined. We use here a novel approach of keeping the singlet quark mass constant in our simulations which upon using an SU(3) flavor symmetry breaking expansion gives highly constrained (i.e. few parameter) fits for hadron masses in a multiplet. This is a highly advantageous procedure for determining the hadron mass gradient as it avoids the use of delicate chiral perturbation theory. We illustrate the procedure here by estimating the light and strange sigma terms for the baryon octet.-
dc.description.statementofresponsibilityR. Horsley, Y. Nakamura, H. Perlt, D. Pleiter, P. E. L. Rakow, G. Schierholz, A. Schiller, H. Stüben, F. Winter, and J. M. Zanotti, (QCDSF-UKQCD Collaboration)-
dc.language.isoen-
dc.publisherAmerican Physical Soc-
dc.rights© 2012 American Physical Society-
dc.source.urihttp://dx.doi.org/10.1103/physrevd.85.034506-
dc.titleHyperon sigma terms for 2+1 quark flavors-
dc.typeJournal article-
dc.identifier.doi10.1103/PhysRevD.85.034506-
pubs.publication-statusPublished-
dc.identifier.orcidZanotti, J. [0000-0002-3936-1597]-
Appears in Collections:Aurora harvest
Chemistry and Physics publications

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