{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:UVAJ6GEF3CFLLVG35EW6ZQIH3C","short_pith_number":"pith:UVAJ6GEF","schema_version":"1.0","canonical_sha256":"a5409f1885d88ab5d4dbe92decc107d889e6b8fb270289c8da7e2afecb83e653","source":{"kind":"arxiv","id":"1408.0458","version":3},"attestation_state":"computed","paper":{"title":"Is $d^*$ a candidate of hexaquark-dominated exotic state?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"F. Huang, P. N. Shen, W. L. Wang, Z. Y. Zhang","submitted_at":"2014-08-03T05:16:54Z","abstract_excerpt":"We confirm our previous prediction of a $d^*$ state with $I(J^P)=0(3^+)$ [Phys. Rev. C 60, 045203 (1999)] and report for the first time based on a microscopic calculation that $d^*$ is a hexaquark dominated exotic state as it has about 2/3 hidden color (CC) configurations. By performing a more elaborate dynamical coupled-channels investigation of the $\\Delta\\Delta$-CC system within the framework of resonating group method (RGM) in a chiral quark model, we found that the $d^*$ state has a mass of about 2.38-2.42 GeV, a root-mean-square radius (RMS) of 0.76-0.88 fm, and a CC fraction of 66%-68%."},"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":"1408.0458","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-08-03T05:16:54Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"4a4d67e97aa96b85af01522bc09b7556aefa3fda2ab7c0f8a3ad5c9423a9de74","abstract_canon_sha256":"3e87786dc03fef89fd5a466dbab8ff9c5e3b86c5fa2e6f62e13e2e7208a7fb9b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:23:58.553305Z","signature_b64":"2Cy1FC4t/9wpGmhAPhv/24kailf0Dfv0RMu8+yMFKN7xN++3JSmQl6sCFmpwxaj+oFcMu9nXCAkO0MJlVbZODA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a5409f1885d88ab5d4dbe92decc107d889e6b8fb270289c8da7e2afecb83e653","last_reissued_at":"2026-05-18T02:23:58.552619Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:23:58.552619Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Is $d^*$ a candidate of hexaquark-dominated exotic state?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"F. Huang, P. N. Shen, W. L. Wang, Z. Y. Zhang","submitted_at":"2014-08-03T05:16:54Z","abstract_excerpt":"We confirm our previous prediction of a $d^*$ state with $I(J^P)=0(3^+)$ [Phys. Rev. C 60, 045203 (1999)] and report for the first time based on a microscopic calculation that $d^*$ is a hexaquark dominated exotic state as it has about 2/3 hidden color (CC) configurations. By performing a more elaborate dynamical coupled-channels investigation of the $\\Delta\\Delta$-CC system within the framework of resonating group method (RGM) in a chiral quark model, we found that the $d^*$ state has a mass of about 2.38-2.42 GeV, a root-mean-square radius (RMS) of 0.76-0.88 fm, and a CC fraction of 66%-68%."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.0458","kind":"arxiv","version":3},"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":"1408.0458","created_at":"2026-05-18T02:23:58.552752+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.0458v3","created_at":"2026-05-18T02:23:58.552752+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.0458","created_at":"2026-05-18T02:23:58.552752+00:00"},{"alias_kind":"pith_short_12","alias_value":"UVAJ6GEF3CFL","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"UVAJ6GEF3CFLLVG3","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"UVAJ6GEF","created_at":"2026-05-18T12:28:52.271510+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C","json":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C.json","graph_json":"https://pith.science/api/pith-number/UVAJ6GEF3CFLLVG35EW6ZQIH3C/graph.json","events_json":"https://pith.science/api/pith-number/UVAJ6GEF3CFLLVG35EW6ZQIH3C/events.json","paper":"https://pith.science/paper/UVAJ6GEF"},"agent_actions":{"view_html":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C","download_json":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C.json","view_paper":"https://pith.science/paper/UVAJ6GEF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.0458&json=true","fetch_graph":"https://pith.science/api/pith-number/UVAJ6GEF3CFLLVG35EW6ZQIH3C/graph.json","fetch_events":"https://pith.science/api/pith-number/UVAJ6GEF3CFLLVG35EW6ZQIH3C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C/action/storage_attestation","attest_author":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C/action/author_attestation","sign_citation":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C/action/citation_signature","submit_replication":"https://pith.science/pith/UVAJ6GEF3CFLLVG35EW6ZQIH3C/action/replication_record"}},"created_at":"2026-05-18T02:23:58.552752+00:00","updated_at":"2026-05-18T02:23:58.552752+00:00"}