{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:4VFBUBU3Y3OPUOZTNSRG4MR6A4","short_pith_number":"pith:4VFBUBU3","schema_version":"1.0","canonical_sha256":"e54a1a069bc6dcfa3b336ca26e323e073199b559344327d1613904bc52007b44","source":{"kind":"arxiv","id":"2009.11983","version":1},"attestation_state":"computed","paper":{"title":"Hexaquark picture for $d^*(2380)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Hungchong Kim, K. S. Kim, Makoto Oka","submitted_at":"2020-09-24T23:55:50Z","abstract_excerpt":"Hexaquark wave function with the quantum numbers $I(J^P)=0(3^+)$, which might be relevant for $d^*(2380)$, is constructed under an assumption that this is composed only of $u,d$ quarks in an $S$-wave. By combining three diquarks of either type, ($\\bm{\\bar{3}}_c, I=1$) or ($\\bm{6}_c, I=0$), we demonstrate that there are five possible configurations for the six-quark state. The fully antisymmetric wave function is constructed by linearly combining the five configurations on an equal footing. We then take this wave function as well as the five configurations to calculate the hexaquark mass using "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2009.11983","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-09-24T23:55:50Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"5ca51cd0b11dc0593c5fdba7e33851fa4cef53e48bda25e397a57680869f5ef0","abstract_canon_sha256":"ff969524896dfd7cd4d4384ca58208f4cb73d7cec74ca61f6b5c73304fee592e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:48:55.460941Z","signature_b64":"mHbTS5ADMYQy1jYMcrJCx0kAY3uUZuBFUKkGLAn9XwdUfaxAbmff2YTynZpLa6rgiWYqgBIMFq8Ej+g+apu3DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e54a1a069bc6dcfa3b336ca26e323e073199b559344327d1613904bc52007b44","last_reissued_at":"2026-07-05T01:48:55.460548Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:48:55.460548Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hexaquark picture for $d^*(2380)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Hungchong Kim, K. S. Kim, Makoto Oka","submitted_at":"2020-09-24T23:55:50Z","abstract_excerpt":"Hexaquark wave function with the quantum numbers $I(J^P)=0(3^+)$, which might be relevant for $d^*(2380)$, is constructed under an assumption that this is composed only of $u,d$ quarks in an $S$-wave. By combining three diquarks of either type, ($\\bm{\\bar{3}}_c, I=1$) or ($\\bm{6}_c, I=0$), we demonstrate that there are five possible configurations for the six-quark state. The fully antisymmetric wave function is constructed by linearly combining the five configurations on an equal footing. We then take this wave function as well as the five configurations to calculate the hexaquark mass using "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2009.11983","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2009.11983/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2009.11983","created_at":"2026-07-05T01:48:55.460611+00:00"},{"alias_kind":"arxiv_version","alias_value":"2009.11983v1","created_at":"2026-07-05T01:48:55.460611+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2009.11983","created_at":"2026-07-05T01:48:55.460611+00:00"},{"alias_kind":"pith_short_12","alias_value":"4VFBUBU3Y3OP","created_at":"2026-07-05T01:48:55.460611+00:00"},{"alias_kind":"pith_short_16","alias_value":"4VFBUBU3Y3OPUOZT","created_at":"2026-07-05T01:48:55.460611+00:00"},{"alias_kind":"pith_short_8","alias_value":"4VFBUBU3","created_at":"2026-07-05T01:48:55.460611+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.01861","citing_title":"Pentaquarks made of light quarks and their admixture to baryons","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4","json":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4.json","graph_json":"https://pith.science/api/pith-number/4VFBUBU3Y3OPUOZTNSRG4MR6A4/graph.json","events_json":"https://pith.science/api/pith-number/4VFBUBU3Y3OPUOZTNSRG4MR6A4/events.json","paper":"https://pith.science/paper/4VFBUBU3"},"agent_actions":{"view_html":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4","download_json":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4.json","view_paper":"https://pith.science/paper/4VFBUBU3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2009.11983&json=true","fetch_graph":"https://pith.science/api/pith-number/4VFBUBU3Y3OPUOZTNSRG4MR6A4/graph.json","fetch_events":"https://pith.science/api/pith-number/4VFBUBU3Y3OPUOZTNSRG4MR6A4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4/action/storage_attestation","attest_author":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4/action/author_attestation","sign_citation":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4/action/citation_signature","submit_replication":"https://pith.science/pith/4VFBUBU3Y3OPUOZTNSRG4MR6A4/action/replication_record"}},"created_at":"2026-07-05T01:48:55.460611+00:00","updated_at":"2026-07-05T01:48:55.460611+00:00"}