{"@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/1361699994397706496.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1016/j.physrep.2016.05.004"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S037015731630103X?httpAccept=text/xml"}},{"identifier":{"@type":"URI","@value":"https://api.elsevier.com/content/article/PII:S037015731630103X?httpAccept=text/plain"}}],"dc:title":[{"@value":"The hidden-charm pentaquark and tetraquark states"}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1381699994397706626","@type":"Researcher","foaf:name":[{"@value":"Hua-Xing Chen"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994397706624","@type":"Researcher","foaf:name":[{"@value":"Wei Chen"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994397706496","@type":"Researcher","foaf:name":[{"@value":"Xiang Liu"}]},{"@id":"https://cir.nii.ac.jp/crid/1381699994397706625","@type":"Researcher","foaf:name":[{"@value":"Shi-Lin Zhu"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"03701573"}],"prism:publicationName":[{"@value":"Physics Reports"}],"dc:publisher":[{"@value":"Elsevier BV"}],"prism:publicationDate":"2016-06","prism:volume":"639","prism:startingPage":"1","prism:endingPage":"121"},"reviewed":"false","dc:rights":["https://www.elsevier.com/tdm/userlicense/1.0/"],"url":[{"@id":"https://api.elsevier.com/content/article/PII:S037015731630103X?httpAccept=text/xml"},{"@id":"https://api.elsevier.com/content/article/PII:S037015731630103X?httpAccept=text/plain"}],"createdAt":"2016-05-31","modifiedAt":"2022-06-29","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050845760787652864","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Structure of hadron resonances with a nearby zero of the amplitude"}]},{"@id":"https://cir.nii.ac.jp/crid/1050848249861109120","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Exotic hadrons from heavy ion collisions"},{"@language":"ja","@value":"重イオン衝突からのエキゾチックハドロン"}]},{"@id":"https://cir.nii.ac.jp/crid/1050860842077943680","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Doubly Charmed Tetraquark ${T}_{cc}^{+}$ from Lattice QCD near Physical Point"},{"@value":"Doubly Charmed Tetraquark \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msubsup><mml:mi>T</mml:mi><mml:mrow><mml:mi>c</mml:mi><mml:mi>c</mml:mi></mml:mrow><mml:mo>+</mml:mo></mml:msubsup></mml:math>\n from Lattice QCD near Physical Point"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235001205120","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Theoretical study of the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mi mathvariant=\"normal\">Ξ</mml:mi><mml:mo>(</mml:mo><mml:mn>1620</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:mi mathvariant=\"normal\">Ξ</mml:mi><mml:mo>(</mml:mo><mml:mn>1690</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math>\n resonances in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mrow><mml:msub><mml:mi mathvariant=\"normal\">Ξ</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mi mathvariant=\"italic\">MB</mml:mi></mml:mrow></mml:math>\n decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235021956736","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msup><mml:mi mathvariant=\"normal\">Λ</mml:mi></mml:mrow></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>D</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:msubsup><mml:mi mathvariant=\"normal\">Λ</mml:mi><mml:mi>c</mml:mi><mml:mo>+</mml:mo></mml:msubsup></mml:math>production induced by pion beams off the nucleon"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235022052608","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>D</mml:mi></mml:math>\n-wave charmed and bottomed baryons from QCD sum rules"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235023667456","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Hidden-charm and bottom meson-baryon molecules coupled with five-quark states"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235023689600","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy molecules and one-\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>σ</mml:mi><mml:mo stretchy=\"false\">/</mml:mo><mml:mi>ω</mml:mi></mml:mrow></mml:math>\n-exchange model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360005519345985280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy hadronic molecules with pion exchange and quark core couplings: a guide for practitioners"}]},{"@id":"https://cir.nii.ac.jp/crid/1360013168856270208","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy Hadronic Molecules Coupled with Multiquark States"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017282195040128","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Evidence for a vector charmoniumlike state in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>e</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>e</mml:mi><mml:mo>−</mml:mo></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:msubsup><mml:mi>D</mml:mi><mml:mi>s</mml:mi><mml:mo>+</mml:mo></mml:msubsup><mml:msubsup><mml:mi>D</mml:mi><mml:mrow><mml:mi>s</mml:mi><mml:mn>2</mml:mn></mml:mrow><mml:mo>*</mml:mo></mml:msubsup><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>2573</mml:mn><mml:msup><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>−</mml:mo></mml:msup><mml:mo>+</mml:mo><mml:mi mathvariant=\"normal\">c</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant=\"normal\">c</mml:mi><mml:mo>.</mml:mo></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360021390561747328","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"50 Years of quantum chromodynamics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360025429411203584","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Nucleon-charmonium interactions from lattice QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1360025431116247040","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Finite volume Hamiltonian method for two-particle systems containing long-range potential on the lattice"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285710000803200","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Flavor-singlet hidden charm pentaquark"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285710000893696","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Searching for possible \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi mathvariant=\"normal\">Ω</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:math>\n-like molecular states from meson-baryon interaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1360294643819552256","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Higher fully charmed tetraquarks: Radial excitations and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>P</mml:mi></mml:math>\n-wave states"}]},{"@id":"https://cir.nii.ac.jp/crid/1360294643866099968","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Near-threshold spectrum from a uniformized Mittag-Leffler expansion: Pole structure of the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>Z</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>3900</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298754829633408","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>S</mml:mi></mml:math>\n-wave fully charmed tetraquark resonant states"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298755610708608","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"First study of the two-body scattering involving charm hadrons"}]},{"@id":"https://cir.nii.ac.jp/crid/1360298755626113152","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Predictions of superexotic heavy mesons from \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>K</mml:mi><mml:mo>*</mml:mo></mml:msup><mml:msup><mml:mi>B</mml:mi><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mo>*</mml:mo><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mi>B</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:math>\n interactions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360302864782298880","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quark model with hidden local symmetry and its application to \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>T</mml:mi><mml:mrow><mml:mi>c</mml:mi><mml:mi>c</mml:mi></mml:mrow></mml:msub></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360306904417375232","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Investigation on the bottom analogs \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi><mml:mi>b</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math>\n of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360306905158084480","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Investigation on the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi mathvariant=\"normal\">Ω</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>2012</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math>\n from QCD sum rules"}]},{"@id":"https://cir.nii.ac.jp/crid/1360306906075912448","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Studying the interaction between charm and light-flavor mesons"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567184976224512","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Decay properties of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>P</mml:mi></mml:mrow></mml:math>\n-wave charmed baryons from light-cone QCD sum rules"}]},{"@id":"https://cir.nii.ac.jp/crid/1360572092802830336","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Positive-Parity Linear-Chain Molecular Band in \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=\"normal\">C</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>16</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360572092876353664","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Photoproduction of \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mover accent=\"true\"><mml:mi>D</mml:mi><mml:mo stretchy=\"false\">¯</mml:mo></mml:mover><mml:mn>0</mml:mn></mml:msup><mml:msubsup><mml:mi mathvariant=\"normal\">Λ</mml:mi><mml:mi>c</mml:mi><mml:mo>+</mml:mo></mml:msubsup></mml:math>\n within the Regge-plus-resonance model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360576118698441088","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy baryon spectrum with chiral multiplets of scalar and vector diquarks"}]},{"@id":"https://cir.nii.ac.jp/crid/1360576118795640320","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Prediction of Double-heavy Tetraquarks Bound States in Quark Model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360576118812103424","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>P</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>4312</mml:mn><mml:msup><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>+</mml:mo></mml:msup></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>4337</mml:mn><mml:msup><mml:mrow><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>\n as interfering \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">Σ</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mover accent=\"true\"><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:math>\n and \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant=\"normal\">Λ</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>\n threshold cusps"}]},{"@id":"https://cir.nii.ac.jp/crid/1360580229815764480","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Open charm and bottom meson-nucleon potentials \n<i>à la</i>\n the nuclear force"}]},{"@id":"https://cir.nii.ac.jp/crid/1360584340702322688","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quark confinement for multiquark systems: Application to fully charmed tetraquarks"}]},{"@id":"https://cir.nii.ac.jp/crid/1360588381061390976","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"New insight into the exotic states strongly coupled with the <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si87.svg\"><mml:mrow><mml:mi>D</mml:mi><mml:msup><mml:mrow><mml:mover accent=\"true\"><mml:mrow><mml:mi>D</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"true\">‾</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mo>∗</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math> from the <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si88.svg\"><mml:mrow><mml:msubsup><mml:mrow><mml:mi>T</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant=\"italic\">cc</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msubsup></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360588381065910144","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Mass spectra of full-heavy and double-heavy tetraquark states in the conventional quark model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848657373512320","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"The hidden charm pentaquarks are the hidden color-octet uud baryons?"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659932368512","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Quark model estimate of hidden-charm pentaquark resonances"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659955529856","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Exotic triple-charm deuteronlike hexaquarks"}]},{"@id":"https://cir.nii.ac.jp/crid/1360849944898944000","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>P</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:math>\n pentaquarks with chiral tensor and quark dynamics"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567344262272","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy baryons in holographic QCD with higher dimensional degrees of freedom"}]},{"@id":"https://cir.nii.ac.jp/crid/1360853567832018432","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Stable double-heavy tetraquarks: Spectrum and structure"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857593773685632","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Doubly heavy tetraquark resonant states"}]},{"@id":"https://cir.nii.ac.jp/crid/1360857597834107136","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Novel pentaquark picture for singly heavy baryons from chiral symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360865815511989632","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Survival probability of unstable states in coupled-channels: Nonexponential decay of threshold cusp"}]},{"@id":"https://cir.nii.ac.jp/crid/1360869855590560000","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Probing exotic \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>J</mml:mi><mml:mrow><mml:mi>P</mml:mi><mml:mi>C</mml:mi></mml:mrow></mml:msup></mml:math>\n resonances from deeply bound charmoniumlike molecules: Insights for identifying exotic hadrons"}]},{"@id":"https://cir.nii.ac.jp/crid/1361131644193776640","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Reliable Design for a Network of Networks with Inspiration from Brain Functional Networks"}]},{"@id":"https://cir.nii.ac.jp/crid/1361412894843559168","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Fate of the charm baryon \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi mathvariant=\"normal\">Λ</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:math>\n in cold and hot nuclear matter"}]},{"@id":"https://cir.nii.ac.jp/crid/1361694369828919168","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Chiral effective theory of diquarks and the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>U</mml:mi><mml:mi>A</mml:mi></mml:msub><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math>\n anomaly"}]},{"@id":"https://cir.nii.ac.jp/crid/2050025942148310528","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Heavy quark spin multiplet structure of Pc-like pentaquarks as a P-wave hadronic molecular state"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842029484544","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Understanding the nature of heavy pentaquarks and searching for them in pion-induced reactions"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842055153280","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Borromean Feshbach resonance in 11Li studied via 11Li(p,p')"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1016/j.physrep.2016.05.004"},{"@type":"CROSSREF","@value":"10.1103/physrevc.95.035212_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.094025_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.94.114016_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.96.114031_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.96.116012_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1088/1361-6471/ab72b0_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2016.11.034_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1007/s00601-021-01614-3_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.101.091101_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1140/epjc/s10052-023-11949-2_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2024.139178_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1007/jhep04(2025)108_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.97.034006_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.97.036016_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1016/j.ppnp.2017.02.002_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.104.036016_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.105.014034_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.106.096005_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.106.052010_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.107.054042_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.3390/app9183809_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.108.054025_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.110.074007_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.110.034007_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.110.032004_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.95.094008_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.97.054019_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.124.192501_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.102.074009_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.104.054012_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1007/s00601-021-01665-6_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.104.l091503_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.106.094001_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevlett.131.161901_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.108.l071501_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1016/j.scib.2024.07.012_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.111.014018_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevc.98.045208_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.97.114011_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.101.091502_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.101.126008_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2021.136095_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1016/j.physletb.2021.136800_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.104.034009_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.108.l071502_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.110.l051501_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz146_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevc.100.065201_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptz126_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.1103/physrevd.101.054038_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"},{"@type":"CROSSREF","@value":"10.7566/jpscp.13.020046_references_DOI_FIFQ9e0rrzMbbVpjtmpEfv9tmIt"}]}