000820961 001__ 820961
000820961 005__ 20240610121034.0
000820961 0247_ $$2doi$$a10.1016/j.nuclphysa.2016.01.006
000820961 0247_ $$2ISSN$$a0375-9474
000820961 0247_ $$2ISSN$$a1873-1554
000820961 0247_ $$2WOS$$aWOS:000381331200018
000820961 0247_ $$2altmetric$$aaltmetric:5075171
000820961 037__ $$aFZJ-2016-06218
000820961 082__ $$a530
000820961 1001_ $$0P:(DE-Juel1)131179$$aHaidenbauer, J.$$b0$$eCorresponding author
000820961 245__ $$aStrangeness S=−2 baryon–baryon interaction at next-to-leading order in chiral effective field theory
000820961 260__ $$aAmsterdam$$bNorth-Holland Publ. Co.$$c2016
000820961 3367_ $$2DRIVER$$aarticle
000820961 3367_ $$2DataCite$$aOutput Types/Journal article
000820961 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1479388003_19616
000820961 3367_ $$2BibTeX$$aARTICLE
000820961 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000820961 3367_ $$00$$2EndNote$$aJournal Article
000820961 520__ $$aThe strangeness S=−2S=−2 baryon–baryon interaction is studied in chiral effective field theory up to next-to-leading order. The potential at this order consists of contributions from one- and two-pseudoscalar-meson exchange diagrams and from four-baryon contact terms without and with two derivatives. SU(3) flavor symmetry is imposed for constructing the interaction in the S=−2S=−2 sector. Specifically, the couplings of the pseudoscalar mesons to the baryons are fixed by SU(3) symmetry and, in general, also the contact terms are related via SU(3) symmetry to those determined in a previous study of the S=−1S=−1 hyperon–nucleon interaction. The explicit SU(3) symmetry breaking due to the physical masses of the pseudoscalar mesons (π, K, η) is taken into account. It is argued that the ΞN   interaction has to be relatively weak to be in accordance with available experimental constraints. In particular, the published values and upper bounds for the Ξ−pΞ−p elastic and inelastic cross sections apparently rule out a somewhat stronger attractive ΞN force and, specifically, disfavor any near-threshold deuteron-like bound states in that system.
000820961 536__ $$0G:(DE-HGF)POF3-511$$a511 - Computational Science and Mathematical Methods (POF3-511)$$cPOF3-511$$fPOF III$$x0
000820961 536__ $$0G:(DE-HGF)POF3-531$$a531 - Condensed Matter and Molecular Building Blocks (POF3-531)$$cPOF3-531$$fPOF III$$x1
000820961 588__ $$aDataset connected to CrossRef
000820961 7001_ $$0P:(DE-Juel1)131252$$aMeißner, Ulf-G.$$b1$$ufzj
000820961 7001_ $$0P:(DE-HGF)0$$aPetschauer, S.$$b2
000820961 773__ $$0PERI:(DE-600)1466542-6$$a10.1016/j.nuclphysa.2016.01.006$$gVol. 954, p. 273 - 293$$p273 - 293$$tNuclear physics <Amsterdam> / A$$v954$$x0375-9474$$y2016
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1-s2.0-S0375947416000075-main.pdf$$yRestricted
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1-s2.0-S0375947416000075-main.gif?subformat=icon$$xicon$$yRestricted
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1-s2.0-S0375947416000075-main.jpg?subformat=icon-1440$$xicon-1440$$yRestricted
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1-s2.0-S0375947416000075-main.jpg?subformat=icon-180$$xicon-180$$yRestricted
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1-s2.0-S0375947416000075-main.jpg?subformat=icon-640$$xicon-640$$yRestricted
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1-s2.0-S0375947416000075-main.pdf?subformat=pdfa$$xpdfa$$yRestricted
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1511.05859.pdf$$yRestricted
000820961 8564_ $$uhttps://juser.fz-juelich.de/record/820961/files/1511.05859.pdf?subformat=pdfa$$xpdfa$$yRestricted
000820961 909CO $$ooai:juser.fz-juelich.de:820961$$pVDB
000820961 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131179$$aForschungszentrum Jülich$$b0$$kFZJ
000820961 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131252$$aForschungszentrum Jülich$$b1$$kFZJ
000820961 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
000820961 9131_ $$0G:(DE-HGF)POF3-531$$1G:(DE-HGF)POF3-530$$2G:(DE-HGF)POF3-500$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bKey Technologies$$lScience and Technology of Nanosystems$$vCondensed Matter and Molecular Building Blocks$$x1
000820961 9141_ $$y2016
000820961 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000820961 915__ $$0StatID:(DE-HGF)0550$$2StatID$$aNo Authors Fulltext
000820961 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search
000820961 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bNUCL PHYS A : 2015
000820961 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000820961 915__ $$0StatID:(DE-HGF)0110$$2StatID$$aWoS$$bScience Citation Index
000820961 915__ $$0StatID:(DE-HGF)0111$$2StatID$$aWoS$$bScience Citation Index Expanded
000820961 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5
000820961 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC
000820961 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences
000820961 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline
000820961 915__ $$0StatID:(DE-HGF)0420$$2StatID$$aNationallizenz
000820961 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bThomson Reuters Master Journal List
000820961 9201_ $$0I:(DE-Juel1)IAS-4-20090406$$kIAS-4$$lTheorie der Starken Wechselwirkung$$x0
000820961 9201_ $$0I:(DE-Juel1)IKP-3-20111104$$kIKP-3$$lTheorie der starken Wechselwirkung$$x1
000820961 980__ $$ajournal
000820961 980__ $$aVDB
000820961 980__ $$aUNRESTRICTED
000820961 980__ $$aI:(DE-Juel1)IAS-4-20090406
000820961 980__ $$aI:(DE-Juel1)IKP-3-20111104
000820961 981__ $$aI:(DE-Juel1)IAS-4-20090406
000820961 981__ $$aI:(DE-Juel1)IKP-3-20111104