{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:MII53FCJKPUM6FOVWGYGPWINUU","short_pith_number":"pith:MII53FCJ","schema_version":"1.0","canonical_sha256":"6211dd944953e8cf15d5b1b067d90da53e9c0953988472b9683d96a75b62e954","source":{"kind":"arxiv","id":"hep-ph/0506270","version":1},"attestation_state":"computed","paper":{"title":"Coupled-channel model for charmonium levels and an option for X(3872)","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Moscow), Yu.S.Kalashnikova (ITEP","submitted_at":"2005-06-27T10:45:22Z","abstract_excerpt":"The effects of charmed meson loops on the spectrum of charmonium are considered, with special attention paid to the levels above open-charm threshold. It is found that the coupling to charmed mesons generates a structure at the D \\bar{D}* threshold in the 1++ partial wave. The implications for the nature of the X(3872) state are discussed."},"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":"hep-ph/0506270","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-06-27T10:45:22Z","cross_cats_sorted":[],"title_canon_sha256":"f1aaca97e48e29101f9aa69ca79261b2400a3f9cdee731e25497c7270a6da255","abstract_canon_sha256":"b07e838a2161c87f4fb89bb2795e373a7365d42461b0f332cf1cf1d6df44833f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:17:45.897043Z","signature_b64":"wtExhO8s1yVtcJnxMgGJhSgO1dvP3NygCR1k9AXBs9wifcKtLQReh2k0H2/HWhJsu7V/aaB8u4hwOZTD1FMbBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6211dd944953e8cf15d5b1b067d90da53e9c0953988472b9683d96a75b62e954","last_reissued_at":"2026-07-04T15:17:45.896632Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:17:45.896632Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Coupled-channel model for charmonium levels and an option for X(3872)","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Moscow), Yu.S.Kalashnikova (ITEP","submitted_at":"2005-06-27T10:45:22Z","abstract_excerpt":"The effects of charmed meson loops on the spectrum of charmonium are considered, with special attention paid to the levels above open-charm threshold. It is found that the coupling to charmed mesons generates a structure at the D \\bar{D}* threshold in the 1++ partial wave. The implications for the nature of the X(3872) state are discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0506270","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/hep-ph/0506270/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":"hep-ph/0506270","created_at":"2026-07-04T15:17:45.896691+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0506270v1","created_at":"2026-07-04T15:17:45.896691+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0506270","created_at":"2026-07-04T15:17:45.896691+00:00"},{"alias_kind":"pith_short_12","alias_value":"MII53FCJKPUM","created_at":"2026-07-04T15:17:45.896691+00:00"},{"alias_kind":"pith_short_16","alias_value":"MII53FCJKPUM6FOV","created_at":"2026-07-04T15:17:45.896691+00:00"},{"alias_kind":"pith_short_8","alias_value":"MII53FCJ","created_at":"2026-07-04T15:17:45.896691+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2604.21403","citing_title":"Comparing relativistic and non-relativistic quark pair creation models","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2604.17193","citing_title":"Proposed mixing between $2P$ and $1F$ wave charmonia","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU","json":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU.json","graph_json":"https://pith.science/api/pith-number/MII53FCJKPUM6FOVWGYGPWINUU/graph.json","events_json":"https://pith.science/api/pith-number/MII53FCJKPUM6FOVWGYGPWINUU/events.json","paper":"https://pith.science/paper/MII53FCJ"},"agent_actions":{"view_html":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU","download_json":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU.json","view_paper":"https://pith.science/paper/MII53FCJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0506270&json=true","fetch_graph":"https://pith.science/api/pith-number/MII53FCJKPUM6FOVWGYGPWINUU/graph.json","fetch_events":"https://pith.science/api/pith-number/MII53FCJKPUM6FOVWGYGPWINUU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU/action/storage_attestation","attest_author":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU/action/author_attestation","sign_citation":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU/action/citation_signature","submit_replication":"https://pith.science/pith/MII53FCJKPUM6FOVWGYGPWINUU/action/replication_record"}},"created_at":"2026-07-04T15:17:45.896691+00:00","updated_at":"2026-07-04T15:17:45.896691+00:00"}