{"@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/1360005520008605312.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevlett.122.242001"}},{"identifier":{"@type":"URI","@value":"https://link.aps.org/article/10.1103/PhysRevLett.122.242001"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevLett.122.242001/fulltext"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1903.11560"}},{"identifier":{"@type":"PMID","@value":"31322380"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Emergence of a Complete Heavy-Quark Spin Symmetry Multiplet: Seven Molecular Pentaquarks in Light of the Latest LHCb Analysis"}],"description":[{"notation":[{"@value":"A recent analysis by the LHCb collaboration suggests the existence of three narrow pentaquark-like states --- the $P_c(4312)$,$P_c(4440)$ and $P_c(4457)$ --- instead of just one in the previous analysis (the $P_c(4450)$). The closeness of the $P_c(4312)$ to the $\\bar{D} ��_c$ threshold and the $P_c(4440)$/$P_c(4457)$ to the $\\bar{D}^* ��_c$ one suggests a molecular interpretation of these resonances. We show that these three pentaquark-like resonances can be naturally accommodated in a contact-range effective field theory description that incorporates heavy-quark spin symmetry. This description leads to the prediction of all the seven possible S-wave heavy antimeson-baryon molecules (that is, there should be four additional molecular pentaquarks in addition to the $P_c(4312)$, $P_c(4440)$ and $P_c(4457)$), providing the first example of a heavy-quark spin symmetry molecular multiplet that is complete. If this is confirmed, it will not only give us an impressive example of the application of heavy-quark symmetries and effective field theories in hadron physics: it will also uncover a clear and powerful ordering principle for the molecular spectrum, reminiscent of the SU(3)-flavor multiplets to which the light hadron spectrum conforms."}]},{"notation":[{"@value":"Corresponds to the version to be published in Physical Review Letters; 4 pages, 1 table summarizing the results, the names of the scenarios have been exchanged to reflect their theoretical preference (scenario A now corresponds to the more likely scenario in pionless EFT)"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380005520008605056","@type":"Researcher","foaf:name":[{"@value":"Ming-Zhu Liu"}]},{"@id":"https://cir.nii.ac.jp/crid/1380005520008605312","@type":"Researcher","foaf:name":[{"@value":"Ya-Wen Pan"}]},{"@id":"https://cir.nii.ac.jp/crid/1380005520008605057","@type":"Researcher","foaf:name":[{"@value":"Fang-Zheng Peng"}]},{"@id":"https://cir.nii.ac.jp/crid/1380005520008605313","@type":"Researcher","foaf:name":[{"@value":"Mario Sánchez Sánchez"}]},{"@id":"https://cir.nii.ac.jp/crid/1380005520008605184","@type":"Researcher","foaf:name":[{"@value":"Li-Sheng 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Bordeaux Gradignan (CENBG)"}]},{"@id":"https://cir.nii.ac.jp/crid/1893962440763982081","@type":"Researcher","foaf:name":[{"@value":"Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"00319007"},{"@type":"EISSN","@value":"10797114"}],"prism:publicationName":[{"@value":"Physical Review Letters"}],"dc:publisher":[{"@value":"American Physical Society 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stretchy=\"false\">(</mml:mo><mml:mn>3872</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math>: Hadronic molecules in effective field theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574096366652672","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Quarkonium Contribution to Meson Molecules"}]},{"@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 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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/1360584340512195968","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Rich structure of the hidden-charm pentaquarks near threshold regions"}]},{"@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/1360855569094199296","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"New Exotic Meson and Baryon Resonances from Doubly Heavy Hadronic Molecules"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569801897600","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Observation of a Charged Charmoniumlike Structure<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>Z</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>4020</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math>and Search for the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>Z</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>3900</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math>in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>e</mml:mi><mml:mo mathvariant=\"bold\">+</mml:mo></mml:msup><mml:msup><mml:mi>e</mml:mi><mml:mo mathvariant=\"bold\">−</mml:mo></mml:msup><mml:mo>→</mml:mo><mml:msup><mml:mi>π</mml:mi><mml:mo mathvariant=\"bold\">+</mml:mo></mml:msup><mml:msup><mml:mi>π</mml:mi><mml:mo mathvariant=\"bold\">−</mml:mo></mml:msup><mml:msub><mml:mi>h</mml:mi><mml:mi>c</mml:mi></mml:msub></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855569877357184","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Implications of Heavy-Quark Spin Symmetry on Heavy-Meson Hadronic Molecules"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855570480087040","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Possible hidden-charm molecular baryons composed of an anti-charmed meson and a charmed baryon"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855570959457920","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mi>Σ</mml:mi><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>¯</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msub><mml:mi>Λ</mml:mi><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>¯</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:math>states in a chiral quark model"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855571444927360","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Testing the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.gif\" overflow=\"scroll\"><mml:msub><mml:mrow><mml:mi>χ</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi><mml:mn>1</mml:mn></mml:mrow></mml:msub><mml:mspace width=\"0.2em\"/><mml:mi>p</mml:mi></mml:math>composite nature of the P c (4450)"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137043481584384","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Diquarks and Exotic Spectroscopy"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418520821607040","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Heavy-quark symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995348745600","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Observation of a Narrow Pentaquark State, \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>4312</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, and of the Two-Peak Structure of the \n<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>4450</mml:mn><mml:msup><mml:mo stretchy=\"false\">)</mml:mo><mml:mo>+</mml:mo></mml:msup></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995391286784","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Formation of hidden-charm pentaquarks in photon-nucleon collisions"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699996197836800","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Towards Exotic Hidden-Charm Pentaquarks in QCD"}]},{"@id":"https://cir.nii.ac.jp/crid/1361975842055197824","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Compact <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" altimg=\"si1.svg\"><mml:mi>s</mml:mi><mml:mi>s</mml:mi><mml:mi>s</mml:mi><mml:mi>c</mml:mi><mml:mover accent=\"true\"><mml:mrow><mml:mi>c</mml:mi></mml:mrow><mml:mrow><mml:mo stretchy=\"false\">¯</mml:mo></mml:mrow></mml:mover></mml:math> pentaquark states predicted by a quark model"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981468519342592","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Heavy-quark spin and flavor symmetry partners of the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>X</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>3872</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:math>\n revisited: What can we learn from the one boson exchange model?"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981469819214208","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Observation of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>J</mml:mi><mml:mo stretchy=\"false\">/</mml:mo><mml:mi>ψ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math>Resonances Consistent with Pentaquark States in<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msubsup><mml:mrow><mml:mi mathvariant=\"normal\">Λ</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msubsup><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>J</mml:mi><mml:mo stretchy=\"false\">/</mml:mo><mml:mi>ψ</mml:mi><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi>p</mml:mi></mml:mrow></mml:math>Decays"}]},{"@id":"https://cir.nii.ac.jp/crid/1361981470339637504","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Amplitude analysis of<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>e</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mo stretchy=\"false\">→</mml:mo><mml:mi mathvariant=\"normal\">ϒ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>n</mml:mi><mml:mi>S</mml:mi><mml:mo stretchy=\"false\">)</mml:mo><mml:msup><mml:mrow><mml:mi>π</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:msup><mml:mrow><mml:mi>π</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>at<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msqrt><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msqrt><mml:mo>=</mml:mo><mml:mn>10.866</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>GeV</mml:mi></mml:mrow></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262943842131968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>J</mml:mi><mml:mo stretchy=\"false\">/</mml:mo><mml:mi>ψ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msub><mml:mrow><mml:mi>η</mml:mi></mml:mrow><mml:mrow><mml:mi>c</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mi>N</mml:mi></mml:mrow></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi mathvariant=\"normal\">ϒ</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:msub><mml:mrow><mml:mi>η</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">)</mml:mo><mml:mi>N</mml:mi></mml:mrow></mml:math>cross sections"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262944463764608","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Dynamically generated<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mi>N</mml:mi><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mi>Λ</mml:mi><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>resonances in the hidden charm sector around 4.3 GeV"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894341919744","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Consequences of heavy-quark symmetries for hadronic molecules"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825894977412608","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Some predictions of diquark model for hidden charm pentaquark discovered at the LHCb"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825895472021248","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Heavy-antiquark–diquark symmetry and heavy hadron molecules: Are there triply heavy pentaquarks?"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825896016316416","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Exotic anti-decuplet of baryons: prediction from chiral solitons"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825896040911232","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Power counting and perturbative one pion exchange in heavy meson 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mathvariant=\"normal\">Λ</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi></mml:mrow></mml:msub><mml:mo stretchy=\"false\">→</mml:mo><mml:mi>J</mml:mi><mml:mo stretchy=\"false\">/</mml:mo><mml:mi>ψ</mml:mi><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi>p</mml:mi></mml:mrow></mml:math>\n reaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107371249938432","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Study of $$P_c(4457)$$, $$P_c(4440)$$, and $$P_c(4312)$$ in a quasipotential Bethe–Salpeter equation approach"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843314024064","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Prediction of Narrow<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>N</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:math>and<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msup><mml:mi>Λ</mml:mi><mml:mo>*</mml:mo></mml:msup></mml:math>Resonances with Hidden Charm above 4 GeV"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843733847936","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Weak decays of heavy mesons in the static quark approximation"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388843888505472","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Scale invariance in heavy hadron molecules"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844560253952","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Heavy quark spin symmetry partners of the<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>X</mml:mi><mml:mo stretchy=\"false\">(</mml:mo><mml:mn>3872</mml:mn><mml:mo 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