{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:OJHZ6RWSIA6WLRECGY575MW6TW","short_pith_number":"pith:OJHZ6RWS","schema_version":"1.0","canonical_sha256":"724f9f46d2403d65c482363bfeb2de9d8c8beefb3d2e377a6926cc27b59afadd","source":{"kind":"arxiv","id":"2002.09401","version":3},"attestation_state":"computed","paper":{"title":"Quark structure of the $\\chi_{\\rm c}(3P)$ and $X(4274)$ resonances and their strong and radiative decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E. Santopinto, J. Ferretti, M. Naeem Anwar, Yu Lu","submitted_at":"2020-02-21T16:35:28Z","abstract_excerpt":"We calculate the masses of $\\chi_{\\rm c}(3P)$ states with threshold corrections in a coupled-channel model. The model was recently applied to the description of the properties of $\\chi_{\\rm c}(2P)$ and $\\chi_{\\rm b}(3P)$ multiplets [Phys.\\ Lett.\\ B {\\bf 789}, 550 (2019)]. We also compute the open-charm strong decay widths of the $\\chi_{\\rm c}(3P)$ states and their radiative transitions. According to our predictions, the $\\chi_{\\rm c}(3P)$ states should be dominated by the charmonium core, but they may also show small meson-meson components. The $X(4274)$ is interpreted as a $c \\bar c$ $\\chi_{\\"},"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":"2002.09401","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-02-21T16:35:28Z","cross_cats_sorted":[],"title_canon_sha256":"402a297cd8adc9067eb0009ddf6e8289bdb67976eebdda630601239ed979b2ee","abstract_canon_sha256":"68ecd593d54a5bb6973ffff94943b98c5e48fcd9a7aff5708c469fd980e150f9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:06:10.218429Z","signature_b64":"NFgg9GIXZetT8K7bZCOXFUPOiVfnyMlgREjzZw7DffvEx1hDsneIpHymUA872t8fb3L3ctMXF7Fxcub30g45Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"724f9f46d2403d65c482363bfeb2de9d8c8beefb3d2e377a6926cc27b59afadd","last_reissued_at":"2026-07-05T01:06:10.217952Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:06:10.217952Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quark structure of the $\\chi_{\\rm c}(3P)$ and $X(4274)$ resonances and their strong and radiative decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E. Santopinto, J. Ferretti, M. Naeem Anwar, Yu Lu","submitted_at":"2020-02-21T16:35:28Z","abstract_excerpt":"We calculate the masses of $\\chi_{\\rm c}(3P)$ states with threshold corrections in a coupled-channel model. The model was recently applied to the description of the properties of $\\chi_{\\rm c}(2P)$ and $\\chi_{\\rm b}(3P)$ multiplets [Phys.\\ Lett.\\ B {\\bf 789}, 550 (2019)]. We also compute the open-charm strong decay widths of the $\\chi_{\\rm c}(3P)$ states and their radiative transitions. According to our predictions, the $\\chi_{\\rm c}(3P)$ states should be dominated by the charmonium core, but they may also show small meson-meson components. The $X(4274)$ is interpreted as a $c \\bar c$ $\\chi_{\\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2002.09401","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2002.09401/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":"2002.09401","created_at":"2026-07-05T01:06:10.218007+00:00"},{"alias_kind":"arxiv_version","alias_value":"2002.09401v3","created_at":"2026-07-05T01:06:10.218007+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2002.09401","created_at":"2026-07-05T01:06:10.218007+00:00"},{"alias_kind":"pith_short_12","alias_value":"OJHZ6RWSIA6W","created_at":"2026-07-05T01:06:10.218007+00:00"},{"alias_kind":"pith_short_16","alias_value":"OJHZ6RWSIA6WLREC","created_at":"2026-07-05T01:06:10.218007+00:00"},{"alias_kind":"pith_short_8","alias_value":"OJHZ6RWS","created_at":"2026-07-05T01:06:10.218007+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/OJHZ6RWSIA6WLRECGY575MW6TW","json":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW.json","graph_json":"https://pith.science/api/pith-number/OJHZ6RWSIA6WLRECGY575MW6TW/graph.json","events_json":"https://pith.science/api/pith-number/OJHZ6RWSIA6WLRECGY575MW6TW/events.json","paper":"https://pith.science/paper/OJHZ6RWS"},"agent_actions":{"view_html":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW","download_json":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW.json","view_paper":"https://pith.science/paper/OJHZ6RWS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2002.09401&json=true","fetch_graph":"https://pith.science/api/pith-number/OJHZ6RWSIA6WLRECGY575MW6TW/graph.json","fetch_events":"https://pith.science/api/pith-number/OJHZ6RWSIA6WLRECGY575MW6TW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW/action/storage_attestation","attest_author":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW/action/author_attestation","sign_citation":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW/action/citation_signature","submit_replication":"https://pith.science/pith/OJHZ6RWSIA6WLRECGY575MW6TW/action/replication_record"}},"created_at":"2026-07-05T01:06:10.218007+00:00","updated_at":"2026-07-05T01:06:10.218007+00:00"}