000889262 001__ 889262
000889262 005__ 20240610121233.0
000889262 0247_ $$2doi$$a10.1103/PhysRevC.101.055502
000889262 0247_ $$2ISSN$$a0556-2813
000889262 0247_ $$2ISSN$$a1089-490X
000889262 0247_ $$2ISSN$$a1538-4497
000889262 0247_ $$2ISSN$$a2469-9985
000889262 0247_ $$2ISSN$$a2469-9993
000889262 0247_ $$2ISSN$$a2470-0002
000889262 0247_ $$2Handle$$a2128/26739
000889262 0247_ $$2altmetric$$aaltmetric:73987757
000889262 0247_ $$2WOS$$aWOS:000530027200005
000889262 037__ $$aFZJ-2021-00167
000889262 082__ $$a530
000889262 1001_ $$0P:(DE-Juel1)131216$$aKrebs, Hermann$$b0$$eCorresponding author
000889262 245__ $$aBox diagram contribution to the axial two-nucleon current
000889262 260__ $$aWoodbury, NY$$bInst.$$c2020
000889262 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2020-05-04
000889262 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2020-05-01
000889262 3367_ $$2DRIVER$$aarticle
000889262 3367_ $$2DataCite$$aOutput Types/Journal article
000889262 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1610471970_22697
000889262 3367_ $$2BibTeX$$aARTICLE
000889262 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000889262 3367_ $$00$$2EndNote$$aJournal Article
000889262 520__ $$aRecently, we have worked out the axial two-nucleon current operator to leading one-loop order in chiral effective field theory using the method of unitary transformation. Our final expressions, however, differ from the ones derived by the JLab-Pisa group using time-ordered perturbation theory [Phys. Rev. C 93, 015501 (2016); Phys. Rev. C 93, 049902(E) (2016); Phys. Rev. C 95, 059901(E) (2017)]. In this paper we consider the box diagram contribution to the axial current and demonstrate that the results obtained using the two methods are unitary equivalent at the Fock-space level. We adjust the unitary phases by matching the corresponding two-pion exchange nucleon-nucleon potentials and rederive the box diagram contribution to the axial current operator following the approach of the JLab-Pisa group, thereby reproducing our original result. We provide a detailed information on the calculation of the box diagram including the relevant intermediate steps in order to facilitate a clarification of this disagreement.
000889262 536__ $$0G:(DE-HGF)POF3-511$$a511 - Computational Science and Mathematical Methods (POF3-511)$$cPOF3-511$$fPOF III$$x0
000889262 536__ $$0G:(GEPRIS)196253076$$aDFG project 196253076 - TRR 110: Symmetrien und Strukturbildung in der Quantenchromodynamik (196253076)$$c196253076$$x1
000889262 542__ $$2Crossref$$i2020-05-04$$uhttps://link.aps.org/licenses/aps-default-license
000889262 588__ $$aDataset connected to CrossRef
000889262 7001_ $$0P:(DE-Juel1)131142$$aEpelbaum, E.$$b1
000889262 7001_ $$0P:(DE-Juel1)131252$$aMeißner, U.-G.$$b2
000889262 77318 $$2Crossref$$3journal-article$$a10.1103/physrevc.101.055502$$bAmerican Physical Society (APS)$$d2020-05-04$$n5$$p055502$$tPhysical Review C$$v101$$x2469-9985$$y2020
000889262 773__ $$0PERI:(DE-600)2844098-5$$a10.1103/PhysRevC.101.055502$$gVol. 101, no. 5, p. 055502$$n5$$p055502$$tPhysical review / C$$v101$$x2469-9985$$y2020
000889262 8564_ $$uhttps://juser.fz-juelich.de/record/889262/files/2001.03904.pdf$$yOpenAccess
000889262 8564_ $$uhttps://juser.fz-juelich.de/record/889262/files/PhysRevC.101.055502.pdf$$yOpenAccess
000889262 909CO $$ooai:juser.fz-juelich.de:889262$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000889262 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131216$$aForschungszentrum Jülich$$b0$$kFZJ
000889262 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131142$$aForschungszentrum Jülich$$b1$$kFZJ
000889262 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131252$$aForschungszentrum Jülich$$b2$$kFZJ
000889262 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
000889262 9141_ $$y2020
000889262 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0160$$2StatID$$aDBCoverage$$bEssential Science Indicators$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)1230$$2StatID$$aDBCoverage$$bCurrent Contents - Electronics and Telecommunications Collection$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search$$d2020-10-13
000889262 915__ $$0LIC:(DE-HGF)APS-112012$$2HGFVOC$$aAmerican Physical Society Transfer of Copyright Agreement
000889262 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0113$$2StatID$$aWoS$$bScience Citation Index Expanded$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000889262 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bPHYS REV C : 2018$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline$$d2020-10-13
000889262 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List$$d2020-10-13
000889262 9201_ $$0I:(DE-Juel1)IAS-4-20090406$$kIAS-4$$lTheorie der Starken Wechselwirkung$$x0
000889262 9201_ $$0I:(DE-Juel1)IKP-3-20111104$$kIKP-3$$lTheorie der starken Wechselwirkung$$x1
000889262 9801_ $$aFullTexts
000889262 980__ $$ajournal
000889262 980__ $$aVDB
000889262 980__ $$aUNRESTRICTED
000889262 980__ $$aI:(DE-Juel1)IAS-4-20090406
000889262 980__ $$aI:(DE-Juel1)IKP-3-20111104
000889262 981__ $$aI:(DE-Juel1)IAS-4-20090406
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/0370-1573(93)90099-Y
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.aop.2017.01.021
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.93.015501
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.93.049902
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.95.059901
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.94.024003
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.95.059902
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.84.024001
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/0375-9474(71)90731-7
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.aop.2004.09.007
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1143/PTP.70.439
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1143/PTP.12.603
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1140/epja/i2007-10496-0
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1007/s00601-019-1500-5
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.60.034002
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.ppnp.2005.09.002
000889262 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.98.044003