{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:ANE6KTDERXL7TI2S6YBHJIWJHM","short_pith_number":"pith:ANE6KTDE","schema_version":"1.0","canonical_sha256":"0349e54c648dd7f9a352f60274a2c93b071af1de00f6603748b0edab2976f20c","source":{"kind":"arxiv","id":"1312.7756","version":1},"attestation_state":"computed","paper":{"title":"Dynamical calculation of the $\\Delta\\Delta$ dibaryon candidates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fan Wang, Hongxia Huang, Jialun Ping","submitted_at":"2013-12-30T16:05:45Z","abstract_excerpt":"We perform a dynamical calculation of the $\\Delta\\Delta$ dibaryon candidates with $IJ^{P}=03^{+}$ and $IJ^{P}=30^{+}$ in the framework of two constituent quark models: the quark delocalization color screening model and the chiral quark model. Our results show that the dibaryon resonances with $IJ^{P}=03^{+}$ and $IJ^{P}=30^{+}$ can be formed in both models. The mass and width of $IJ^{P}=03^{+}$ state are smaller than that of $IJ^{P}=30^{+}$ state due to the one-gluon-exchange interaction between quarks. The resonance mass and decay width of $IJ^{P}=03^{+}$ state in both models agree with that "},"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":"1312.7756","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-12-30T16:05:45Z","cross_cats_sorted":[],"title_canon_sha256":"837fc634c18bb77a9d5a55cf04d219166327dd3d15e05f4e59984fb864d8450f","abstract_canon_sha256":"152878b407c6868d62bfc3738a4d042ca6ec71000337bcedd8b402f78c704d34"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:43.585086Z","signature_b64":"y6pXhxGMjCtaI6kWJvFXxU8ChMPCGYWYJaSFYm8CxhIZSS2k+6IZzMYPoqTPouSycK6edZCMrWxt/Q1N3gWOBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0349e54c648dd7f9a352f60274a2c93b071af1de00f6603748b0edab2976f20c","last_reissued_at":"2026-05-18T02:56:43.584628Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:43.584628Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical calculation of the $\\Delta\\Delta$ dibaryon candidates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fan Wang, Hongxia Huang, Jialun Ping","submitted_at":"2013-12-30T16:05:45Z","abstract_excerpt":"We perform a dynamical calculation of the $\\Delta\\Delta$ dibaryon candidates with $IJ^{P}=03^{+}$ and $IJ^{P}=30^{+}$ in the framework of two constituent quark models: the quark delocalization color screening model and the chiral quark model. Our results show that the dibaryon resonances with $IJ^{P}=03^{+}$ and $IJ^{P}=30^{+}$ can be formed in both models. The mass and width of $IJ^{P}=03^{+}$ state are smaller than that of $IJ^{P}=30^{+}$ state due to the one-gluon-exchange interaction between quarks. The resonance mass and decay width of $IJ^{P}=03^{+}$ state in both models agree with that "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.7756","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":""},"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":"1312.7756","created_at":"2026-05-18T02:56:43.584690+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.7756v1","created_at":"2026-05-18T02:56:43.584690+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.7756","created_at":"2026-05-18T02:56:43.584690+00:00"},{"alias_kind":"pith_short_12","alias_value":"ANE6KTDERXL7","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"ANE6KTDERXL7TI2S","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"ANE6KTDE","created_at":"2026-05-18T12:27:38.830355+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.10660","citing_title":"Lattice QCD Study of Positive Parity Dibaryons with Maximal Charm and Strangeness","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM","json":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM.json","graph_json":"https://pith.science/api/pith-number/ANE6KTDERXL7TI2S6YBHJIWJHM/graph.json","events_json":"https://pith.science/api/pith-number/ANE6KTDERXL7TI2S6YBHJIWJHM/events.json","paper":"https://pith.science/paper/ANE6KTDE"},"agent_actions":{"view_html":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM","download_json":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM.json","view_paper":"https://pith.science/paper/ANE6KTDE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.7756&json=true","fetch_graph":"https://pith.science/api/pith-number/ANE6KTDERXL7TI2S6YBHJIWJHM/graph.json","fetch_events":"https://pith.science/api/pith-number/ANE6KTDERXL7TI2S6YBHJIWJHM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM/action/storage_attestation","attest_author":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM/action/author_attestation","sign_citation":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM/action/citation_signature","submit_replication":"https://pith.science/pith/ANE6KTDERXL7TI2S6YBHJIWJHM/action/replication_record"}},"created_at":"2026-05-18T02:56:43.584690+00:00","updated_at":"2026-05-18T02:56:43.584690+00:00"}