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Please use this identifier to cite or link to this item: https://hdl.handle.net/2440/76498
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dc.contributor.authorBietenholz, W.-
dc.contributor.authorGockeler, M.-
dc.contributor.authorHorsley, R.-
dc.contributor.authorNakamura, Y.-
dc.contributor.authorPleiter, D.-
dc.contributor.authorRakow, P.-
dc.contributor.authorSchierholz, G.-
dc.contributor.authorZanotti, J.-
dc.date.issued2010-
dc.identifier.citationPhysics Letters B: Nuclear Physics and Particle Physics, 2010; 687(4-5):410-414-
dc.identifier.issn0370-2693-
dc.identifier.issn1873-2445-
dc.identifier.urihttp://hdl.handle.net/2440/76498-
dc.description.abstractThe residual mass of the pion in a finite spatial box at vanishing quark masses, the mass gap, is computed with two flavors of dynamical clover fermions. The result is compared with predictions of chiral perturbation theory in the δ regime. © 2010 Elsevier B.V. All rights reserved.-
dc.description.statementofresponsibilityQCDSF Collaboration, W. Bietenholz, M. Göckeler, R. Horsley, Y. Nakamura, D. Pleiter, P.E.L. Rakow, G. Schierholz, J.M. Zanotti-
dc.language.isoen-
dc.publisherElsevier Science BV-
dc.rights© 2010 Elsevier B.V. All rights reserved.-
dc.source.urihttp://dx.doi.org/10.1016/j.physletb.2010.03.063-
dc.subjectLattice QCD-
dc.subjectChiral perturbation theory-
dc.subjectFinite volume-
dc.titlePion in a box-
dc.typeJournal article-
dc.identifier.doi10.1016/j.physletb.2010.03.063-
pubs.publication-statusPublished-
dc.identifier.orcidZanotti, J. [0000-0002-3936-1597]-
Appears in Collections:Aurora harvest
Chemistry and Physics publications

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