{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:AGF3GN5AA7GIOIK2MO2P25AF7B","short_pith_number":"pith:AGF3GN5A","schema_version":"1.0","canonical_sha256":"018bb337a007cc87215a63b4fd7405f858b7e1ca10f865b15fb60e6a66f3770e","source":{"kind":"arxiv","id":"1510.08305","version":3},"attestation_state":"computed","paper":{"title":"Properties of Excited Charm and Charm-Strange Mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Kenneth Moats (Carleton University), Stephen Godfrey","submitted_at":"2015-10-28T13:42:07Z","abstract_excerpt":"We calculate the properties of excited charm and charm-strange mesons. We use the relativized quark model to calculate their masses and wavefunctions that are used to calculate radiative transition partial widths and the $^3P_0$ quark-pair-creation model to calculate their strong decay widths. We use these results to make quark model spectroscopic assignments for recently observed charm and charm-strange mesons. In particular we find that the properties of the $D_J(2550)^0$ and $D_J^*(2600)^0$ are consistent with those of the $2^1S_0(c\\bar{u})$ and the $2^3S_1(c\\bar{u})$ states respectively, t"},"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":"1510.08305","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-10-28T13:42:07Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"33e0eab11baf2761b64f8758d293a30a6d3b573848bdfa50731e45f4b2272bbf","abstract_canon_sha256":"987edb325cde918162f6275888d4a07e5b6fa32e6a665d3a5f41a19439f59be5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:47.877995Z","signature_b64":"3MbbCVZELTp+hdZK2mFlFuglZ8aGQ29Tqm+KKNJfaCgA82Pcn60IBK7PpDo+Q8CgqKVV4VhNbwLqiKDigZ51Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"018bb337a007cc87215a63b4fd7405f858b7e1ca10f865b15fb60e6a66f3770e","last_reissued_at":"2026-05-18T01:19:47.877616Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:47.877616Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Properties of Excited Charm and Charm-Strange Mesons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Kenneth Moats (Carleton University), Stephen Godfrey","submitted_at":"2015-10-28T13:42:07Z","abstract_excerpt":"We calculate the properties of excited charm and charm-strange mesons. We use the relativized quark model to calculate their masses and wavefunctions that are used to calculate radiative transition partial widths and the $^3P_0$ quark-pair-creation model to calculate their strong decay widths. We use these results to make quark model spectroscopic assignments for recently observed charm and charm-strange mesons. In particular we find that the properties of the $D_J(2550)^0$ and $D_J^*(2600)^0$ are consistent with those of the $2^1S_0(c\\bar{u})$ and the $2^3S_1(c\\bar{u})$ states respectively, t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.08305","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":"1510.08305","created_at":"2026-05-18T01:19:47.877671+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.08305v3","created_at":"2026-05-18T01:19:47.877671+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.08305","created_at":"2026-05-18T01:19:47.877671+00:00"},{"alias_kind":"pith_short_12","alias_value":"AGF3GN5AA7GI","created_at":"2026-05-18T12:29:10.953037+00:00"},{"alias_kind":"pith_short_16","alias_value":"AGF3GN5AA7GIOIK2","created_at":"2026-05-18T12:29:10.953037+00:00"},{"alias_kind":"pith_short_8","alias_value":"AGF3GN5A","created_at":"2026-05-18T12:29:10.953037+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2605.17832","citing_title":"Higher excited charmed and charmed-strange mesons in an unquenched quark model","ref_index":41,"is_internal_anchor":true},{"citing_arxiv_id":"2605.18075","citing_title":"Compact $cs\\bar{s}\\bar{s}$ Tetraquarks in the Charm--Strange Sector: Mass Spectra, Rearrangement Decays and Regge Trajectories with $D_s$ Threshold Inputs","ref_index":49,"is_internal_anchor":true},{"citing_arxiv_id":"2511.12996","citing_title":"Radiative Decays of Vector Mesons with Light-Cone Sum Rules","ref_index":21,"is_internal_anchor":true},{"citing_arxiv_id":"2604.21257","citing_title":"Observation of a new excited charm-strange meson $D_{s1}(2933)^+$ in $B^0\\to D^+ D^- K^+ \\pi^-$ decays","ref_index":3,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03021","citing_title":"Closing the knowledge gap in semileptonic $B\\rightarrow X_c\\ell\\nu$ decays","ref_index":57,"is_internal_anchor":false},{"citing_arxiv_id":"2604.18286","citing_title":"Analysis of the $D_0^*(2300)$ resonance from lattice QCD under chiral symmetry","ref_index":10,"is_internal_anchor":false},{"citing_arxiv_id":"2604.17193","citing_title":"Proposed mixing between $2P$ and $1F$ wave charmonia","ref_index":49,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B","json":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B.json","graph_json":"https://pith.science/api/pith-number/AGF3GN5AA7GIOIK2MO2P25AF7B/graph.json","events_json":"https://pith.science/api/pith-number/AGF3GN5AA7GIOIK2MO2P25AF7B/events.json","paper":"https://pith.science/paper/AGF3GN5A"},"agent_actions":{"view_html":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B","download_json":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B.json","view_paper":"https://pith.science/paper/AGF3GN5A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.08305&json=true","fetch_graph":"https://pith.science/api/pith-number/AGF3GN5AA7GIOIK2MO2P25AF7B/graph.json","fetch_events":"https://pith.science/api/pith-number/AGF3GN5AA7GIOIK2MO2P25AF7B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B/action/storage_attestation","attest_author":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B/action/author_attestation","sign_citation":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B/action/citation_signature","submit_replication":"https://pith.science/pith/AGF3GN5AA7GIOIK2MO2P25AF7B/action/replication_record"}},"created_at":"2026-05-18T01:19:47.877671+00:00","updated_at":"2026-05-18T01:19:47.877671+00:00"}