000817800 001__ 817800
000817800 005__ 20210129224029.0
000817800 0247_ $$2doi$$a10.1103/PhysRevLett.117.082001
000817800 0247_ $$2ISSN$$a0031-9007
000817800 0247_ $$2ISSN$$a1079-7114
000817800 0247_ $$2Handle$$a2128/12218
000817800 0247_ $$2WOS$$aWOS:000381495100005
000817800 0247_ $$2altmetric$$aaltmetric:6956926
000817800 0247_ $$2pmid$$apmid:27588847
000817800 037__ $$aFZJ-2016-04440
000817800 082__ $$a550
000817800 1001_ $$0P:(DE-HGF)0$$aFodor, Z.$$b0
000817800 245__ $$aUp and Down Quark Masses and Corrections to Dashen’s Theorem from Lattice QCD and Quenched QED
000817800 260__ $$aCollege Park, Md.$$bAPS$$c2016
000817800 3367_ $$2DRIVER$$aarticle
000817800 3367_ $$2DataCite$$aOutput Types/Journal article
000817800 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1502262713_32598
000817800 3367_ $$2BibTeX$$aARTICLE
000817800 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000817800 3367_ $$00$$2EndNote$$aJournal Article
000817800 520__ $$aIn a previous Letter [Borsanyi et al., Phys. Rev. Lett. 111, 252001 (2013)] we determined the isospin mass splittings of the baryon octet from a lattice calculation based on Nf=2+1 QCD simulations to which QED effects have been added in a partially quenched setup. Using the same data we determine here the corrections to Dashen’s theorem and the individual up and down quark masses. Our ensembles include 5 lattice spacings down to 0.054 fm, lattice sizes up to 6 fm, and average up-down quark masses all the way down to their physical value. For the parameter which quantifies violations to Dashen’s theorem, we obtain ϵ=0.73(2)(5)(17), where the first error is statistical, the second is systematic, and the third is an estimate of the QED quenching error. For the light quark masses we obtain, mu=2.27(6)(5)(4) and md=4.67(6)(5)(4)  MeV in the modified minimal subtraction scheme at 2  GeV and the isospin breaking ratios mu/md=0.485(11)(8)(14), R=38.2(1.1)(0.8)(1.4), and Q=23.4(0.4)(0.3)(0.4). Our results exclude the mu=0 solution to the strong CP problem by more than 24 standard deviations.
000817800 536__ $$0G:(DE-HGF)POF3-511$$a511 - Computational Science and Mathematical Methods (POF3-511)$$cPOF3-511$$fPOF III$$x0
000817800 536__ $$0G:(DE-Juel1)hjs00_20151101$$aUp and down quark masses from lattice QCD + QED (hjs00_20151101)$$chjs00_20151101$$fUp and down quark masses from lattice QCD + QED$$x1
000817800 588__ $$aDataset connected to CrossRef
000817800 7001_ $$0P:(DE-HGF)0$$aHoelbling, C.$$b1
000817800 7001_ $$0P:(DE-Juel1)132171$$aKrieg, S.$$b2$$ufzj
000817800 7001_ $$0P:(DE-HGF)0$$aLellouch, L.$$b3
000817800 7001_ $$0P:(DE-Juel1)132179$$aLippert, Th.$$b4$$ufzj
000817800 7001_ $$0P:(DE-HGF)0$$aPortelli, A.$$b5
000817800 7001_ $$0P:(DE-HGF)0$$aSastre, A.$$b6
000817800 7001_ $$0P:(DE-Juel1)161563$$aSzabo, Kalman$$b7$$ufzj
000817800 7001_ $$0P:(DE-HGF)0$$aVarnhorst, L.$$b8
000817800 773__ $$0PERI:(DE-600)1472655-5$$a10.1103/PhysRevLett.117.082001$$gVol. 117, no. 8, p. 082001$$n8$$p082001$$tPhysical review letters$$v117$$x1079-7114$$y2016
000817800 8564_ $$uhttps://juser.fz-juelich.de/record/817800/files/PhysRevLett.117.082001.pdf$$yOpenAccess
000817800 8564_ $$uhttps://juser.fz-juelich.de/record/817800/files/PhysRevLett.117.082001.gif?subformat=icon$$xicon$$yOpenAccess
000817800 8564_ $$uhttps://juser.fz-juelich.de/record/817800/files/PhysRevLett.117.082001.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess
000817800 8564_ $$uhttps://juser.fz-juelich.de/record/817800/files/PhysRevLett.117.082001.jpg?subformat=icon-180$$xicon-180$$yOpenAccess
000817800 8564_ $$uhttps://juser.fz-juelich.de/record/817800/files/PhysRevLett.117.082001.jpg?subformat=icon-640$$xicon-640$$yOpenAccess
000817800 8564_ $$uhttps://juser.fz-juelich.de/record/817800/files/PhysRevLett.117.082001.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000817800 909CO $$ooai:juser.fz-juelich.de:817800$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire
000817800 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)132171$$aForschungszentrum Jülich$$b2$$kFZJ
000817800 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)132179$$aForschungszentrum Jülich$$b4$$kFZJ
000817800 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)161563$$aForschungszentrum Jülich$$b7$$kFZJ
000817800 9131_ $$0G:(DE-HGF)POF3-511$$1G:(DE-HGF)POF3-510$$2G:(DE-HGF)POF3-500$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bKey Technologies$$lSupercomputing & Big Data$$vComputational Science and Mathematical Methods$$x0
000817800 9141_ $$y2016
000817800 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000817800 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search
000817800 915__ $$0LIC:(DE-HGF)APS-112012$$2HGFVOC$$aAmerican Physical Society Transfer of Copyright Agreement
000817800 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bPHYS REV LETT : 2015
000817800 915__ $$0StatID:(DE-HGF)9905$$2StatID$$aIF >= 5$$bPHYS REV LETT : 2015
000817800 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000817800 915__ $$0StatID:(DE-HGF)0110$$2StatID$$aWoS$$bScience Citation Index
000817800 915__ $$0StatID:(DE-HGF)0111$$2StatID$$aWoS$$bScience Citation Index Expanded
000817800 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000817800 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC
000817800 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences
000817800 915__ $$0StatID:(DE-HGF)0310$$2StatID$$aDBCoverage$$bNCBI Molecular Biology Database
000817800 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline
000817800 915__ $$0StatID:(DE-HGF)0420$$2StatID$$aNationallizenz
000817800 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bThomson Reuters Master Journal List
000817800 920__ $$lyes
000817800 9201_ $$0I:(DE-Juel1)JSC-20090406$$kJSC$$lJülich Supercomputing Center$$x0
000817800 9201_ $$0I:(DE-Juel1)NIC-20090406$$kNIC$$lJohn von Neumann - Institut für Computing$$x1
000817800 980__ $$ajournal
000817800 980__ $$aVDB
000817800 980__ $$aI:(DE-Juel1)JSC-20090406
000817800 980__ $$aI:(DE-Juel1)NIC-20090406
000817800 980__ $$aUNRESTRICTED
000817800 9801_ $$aFullTexts