{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1362262943350907392.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/j.nuclphysa.2012.01.029"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0375947412000607?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S0375947412000607?httpAccept=text/plain"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1201.6549"}},{"identifier":{"@type":"HANDLE","@value":"11582/302753"}}],"dc:title":[{"@value":"Chiral SU(3) theory of antikaon–nucleon interactions with improved threshold constraints"}],"description":[{"notation":[{"@value":"$\\bar{K}$-nucleon interactions are investigated in the framework of coupled-channels dynamics based on the next-to-leading order chiral SU(3) meson-baryon effective Lagrangian. A recent determination of the 1s shift and width of kaonic hydrogen enables us to set accurate constraints on the coupled-channels meson-baryon amplitudes in the strangeness $S=-1$ sector. Theoretical uncertainties in the subthreshold extrapolation of the coupled-channels amplitudes are discussed. Using this framework, we give predictions for $K^-$-neutron interactions and for the spectrum of the $��(1405)$ resonance. A simplified, effective three-channel model using leading order chiral SU(3) meson-baryon interactions is also constructed for convenient application in $\\bar{K}$-nuclear few-body calculations."}]},{"notation":[{"@value":"24 pages, 7 figures"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1382262943350907394","@type":"Researcher","foaf:name":[{"@value":"Yoichi Ikeda"}]},{"@id":"https://cir.nii.ac.jp/crid/1420845751164206080","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"60539823"},{"@type":"NRID","@value":"1000060539823"},{"@type":"CINII_AUTHOR_ID","@value":"DB00107599"},{"@type":"URI","@value":"https://ci.nii.ac.jp/author/DB00107599#entity"},{"@type":"URI","@value":"https://viaf.org/viaf/NII%7CDB00107599"},{"@type":"NRID","@value":"9000003433536"},{"@type":"NRID","@value":"9000241967417"},{"@type":"NRID","@value":"9000376930153"},{"@type":"NRID","@value":"9000402474533"},{"@type":"NRID","@value":"9000390430750"},{"@type":"NRID","@value":"9000351485880"},{"@type":"NRID","@value":"9000367024485"},{"@type":"NRID","@value":"9000401949975"},{"@type":"NRID","@value":"9000351496102"},{"@type":"NRID","@value":"9000274301170"},{"@type":"NRID","@value":"9000401950926"},{"@type":"NRID","@value":"9000364782948"},{"@type":"NRID","@value":"9000376928809"},{"@type":"NRID","@value":"9000415113177"},{"@type":"NRID","@value":"9000333209966"},{"@type":"NRID","@value":"9000333087201"},{"@type":"NRID","@value":"9000403821148"},{"@type":"NRID","@value":"9000401916046"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/tetsuohyodo"}],"foaf:name":[{"@value":"Tetsuo Hyodo"}]},{"@id":"https://cir.nii.ac.jp/crid/1382262943350907392","@type":"Researcher","foaf:name":[{"@value":"Wolfram Weise"}]}],"contributor":[{"@id":"https://cir.nii.ac.jp/crid/1893399490758982528","@type":"Researcher","foaf:name":[{"@value":"Weise, Wolfram"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"03759474"},{"@type":"PISSN","@value":"http://id.crossref.org/issn/03759474"}],"prism:publicationName":[{"@value":"Nuclear Physics A"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"2012-05","prism:volume":"881","prism:startingPage":"98","prism:endingPage":"114"},"reviewed":"false","dcterms:accessRights":"http://purl.org/coar/access_right/c_abf2","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:S0375947412000607?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:S0375947412000607?httpAccept=text/plain"}],"createdAt":"2012-02-03","modifiedAt":"2019-06-23","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20Theory%20(nucl-th)","dc:title":"Nuclear Theory (nucl-th)"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology","dc:title":"High Energy Physics - Phenomenology"},{"@id":"https://cir.nii.ac.jp/all?q=High%20Energy%20Physics%20-%20Phenomenology%20(hep-ph)","dc:title":"High Energy Physics - Phenomenology (hep-ph)"},{"@id":"https://cir.nii.ac.jp/all?q=Nuclear%20Theory","dc:title":"Nuclear Theory"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050282810814999808","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Comprehensive analysis of the wave function of a hadronic resonance and its compositeness"}]},{"@id":"https://cir.nii.ac.jp/crid/1050282810828607488","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Generalized weak-binding relations of compositeness in effective field theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1050564285750290176","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Hadronic Few-Body Systems in Chiral 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