{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:X7CGUI6QVZB6JDDCKRL42UP5N4","short_pith_number":"pith:X7CGUI6Q","schema_version":"1.0","canonical_sha256":"bfc46a23d0ae43e48c625457cd51fd6f23cc888747f832f423cf32d34b81d68c","source":{"kind":"arxiv","id":"2209.13856","version":2},"attestation_state":"computed","paper":{"title":"Spectrum of the S-wave fully-heavy tetraquark states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cheng-Rong Deng, Chun-Sheng An, Gang Li, Jie Zhang, Jin-Bao Wang, Ju-Jun Xie","submitted_at":"2022-09-28T06:24:48Z","abstract_excerpt":"In present work, spectrum of the $S$-wave fully-heavy tetraquark states $QQ\\bar{Q}\\bar{Q}$ ($Q=c,b$), i.e., $cc\\bar{c}\\bar{c}$, $bb\\bar{b}\\bar{b}$, $cc\\bar{b}\\bar{b}$/$bb\\bar{c}\\bar{c}$, $bc\\bar{c}\\bar{c}$/ $cc\\bar{b}\\bar{c}$, $bb\\bar{c}\\bar{b}$/$cb\\bar{b}\\bar{b}$, and $bc\\bar{b}\\bar{c}$ are systematically investigated within an nonrelativistic constituent quark model, in which the Instanton-induced and one-gluon-exchange interactions are taken into account as the residual spin-dependent hyperfine interaction. Our results show that the states with $cc\\bar{c}\\bar{c}$ and $bb\\bar{b}\\bar{b}$ comp"},"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":"2209.13856","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-09-28T06:24:48Z","cross_cats_sorted":[],"title_canon_sha256":"1ebc956d2def8f06550e632a4511c46f168dad503284e6865fe61abfa69db808","abstract_canon_sha256":"badb444f145fc1e7f36fd87f50784bbb2ec6ad09e84605d1f4c73d3b630787ec"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:28:29.103062Z","signature_b64":"ZWhHb1h1dZyMbd3Otehb2KB+jc0gzuxbiZNq0i6Khe85LEkMK3hd7TgrvU/BkIrbrTulCpiGB4p1D8tBjiZyBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bfc46a23d0ae43e48c625457cd51fd6f23cc888747f832f423cf32d34b81d68c","last_reissued_at":"2026-07-05T05:28:29.102581Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:28:29.102581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spectrum of the S-wave fully-heavy tetraquark states","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cheng-Rong Deng, Chun-Sheng An, Gang Li, Jie Zhang, Jin-Bao Wang, Ju-Jun Xie","submitted_at":"2022-09-28T06:24:48Z","abstract_excerpt":"In present work, spectrum of the $S$-wave fully-heavy tetraquark states $QQ\\bar{Q}\\bar{Q}$ ($Q=c,b$), i.e., $cc\\bar{c}\\bar{c}$, $bb\\bar{b}\\bar{b}$, $cc\\bar{b}\\bar{b}$/$bb\\bar{c}\\bar{c}$, $bc\\bar{c}\\bar{c}$/ $cc\\bar{b}\\bar{c}$, $bb\\bar{c}\\bar{b}$/$cb\\bar{b}\\bar{b}$, and $bc\\bar{b}\\bar{c}$ are systematically investigated within an nonrelativistic constituent quark model, in which the Instanton-induced and one-gluon-exchange interactions are taken into account as the residual spin-dependent hyperfine interaction. Our results show that the states with $cc\\bar{c}\\bar{c}$ and $bb\\bar{b}\\bar{b}$ comp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.13856","kind":"arxiv","version":2},"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/2209.13856/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":"2209.13856","created_at":"2026-07-05T05:28:29.102634+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.13856v2","created_at":"2026-07-05T05:28:29.102634+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.13856","created_at":"2026-07-05T05:28:29.102634+00:00"},{"alias_kind":"pith_short_12","alias_value":"X7CGUI6QVZB6","created_at":"2026-07-05T05:28:29.102634+00:00"},{"alias_kind":"pith_short_16","alias_value":"X7CGUI6QVZB6JDDC","created_at":"2026-07-05T05:28:29.102634+00:00"},{"alias_kind":"pith_short_8","alias_value":"X7CGUI6Q","created_at":"2026-07-05T05:28:29.102634+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.24380","citing_title":"Fully-heavy multiquarks in neural-network quantum states","ref_index":73,"is_internal_anchor":false},{"citing_arxiv_id":"2503.00552","citing_title":"Study of $1^{--}$ P wave charmoniumlike and bottomoniumlike tetraquark spectroscopy","ref_index":46,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4","json":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4.json","graph_json":"https://pith.science/api/pith-number/X7CGUI6QVZB6JDDCKRL42UP5N4/graph.json","events_json":"https://pith.science/api/pith-number/X7CGUI6QVZB6JDDCKRL42UP5N4/events.json","paper":"https://pith.science/paper/X7CGUI6Q"},"agent_actions":{"view_html":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4","download_json":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4.json","view_paper":"https://pith.science/paper/X7CGUI6Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.13856&json=true","fetch_graph":"https://pith.science/api/pith-number/X7CGUI6QVZB6JDDCKRL42UP5N4/graph.json","fetch_events":"https://pith.science/api/pith-number/X7CGUI6QVZB6JDDCKRL42UP5N4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4/action/storage_attestation","attest_author":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4/action/author_attestation","sign_citation":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4/action/citation_signature","submit_replication":"https://pith.science/pith/X7CGUI6QVZB6JDDCKRL42UP5N4/action/replication_record"}},"created_at":"2026-07-05T05:28:29.102634+00:00","updated_at":"2026-07-05T05:28:29.102634+00:00"}