{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:NKK32KZSHONEODUE4PHY36YTZA","short_pith_number":"pith:NKK32KZS","schema_version":"1.0","canonical_sha256":"6a95bd2b323b9a470e84e3cf8dfb13c83770668b90bd59c452e7e76703b3aa6c","source":{"kind":"arxiv","id":"1409.0874","version":3},"attestation_state":"computed","paper":{"title":"The $D_{sJ}^*(2860)$ Mesons as Excited D-wave $c\\bar{s}$ States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Kenneth Moats (Carleton University), Stephen Godfrey","submitted_at":"2014-09-02T20:14:28Z","abstract_excerpt":"A new charm-strange meson, the $D_{s1}^*(2863)$, has recently been observed by the LHCb collaboration which also determined the $D_{sJ}^*(2860)$ to have spin 3. One of the speculations about the previously observed $D_{s1}^*(2710)$ is that it is the $1^3D_1(c\\bar{s})$ state. In this paper we reexamine the quark model properties and assignments of these three states in light of these new measurements. We conclude that the $D_{s1}^*(2863)$ and $D_{s3}^*(2863)$ are the $1^3D_1 (c\\bar{s})$ and $1^3D_3 (c\\bar{s})$ states respectively and the $D_{s1}^*(2710)$ is the $2^3S_1(c\\bar{s})$ state. In addi"},"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":"1409.0874","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-09-02T20:14:28Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"c8c6d7e47963a09e77ddb2b022a3d2d2021ece92d5525d467d70dce08a2ad171","abstract_canon_sha256":"91f38f7b9d60eafa4da2d283a9319ba3ec62024beb5e3a9edf6870e09e2009fb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:27:46.558028Z","signature_b64":"NwfWM00SCJpOx6ZuUzy8x1ogiArlgxLalgQqj5aDKgVdihbZESlqPrgMm0Cp2zE5WU5yyU4Aepg2khFeK2HuAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a95bd2b323b9a470e84e3cf8dfb13c83770668b90bd59c452e7e76703b3aa6c","last_reissued_at":"2026-05-18T01:27:46.557492Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:27:46.557492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The $D_{sJ}^*(2860)$ Mesons as Excited D-wave $c\\bar{s}$ States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Kenneth Moats (Carleton University), Stephen Godfrey","submitted_at":"2014-09-02T20:14:28Z","abstract_excerpt":"A new charm-strange meson, the $D_{s1}^*(2863)$, has recently been observed by the LHCb collaboration which also determined the $D_{sJ}^*(2860)$ to have spin 3. One of the speculations about the previously observed $D_{s1}^*(2710)$ is that it is the $1^3D_1(c\\bar{s})$ state. In this paper we reexamine the quark model properties and assignments of these three states in light of these new measurements. We conclude that the $D_{s1}^*(2863)$ and $D_{s3}^*(2863)$ are the $1^3D_1 (c\\bar{s})$ and $1^3D_3 (c\\bar{s})$ states respectively and the $D_{s1}^*(2710)$ is the $2^3S_1(c\\bar{s})$ state. In addi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.0874","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":"1409.0874","created_at":"2026-05-18T01:27:46.557578+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.0874v3","created_at":"2026-05-18T01:27:46.557578+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.0874","created_at":"2026-05-18T01:27:46.557578+00:00"},{"alias_kind":"pith_short_12","alias_value":"NKK32KZSHONE","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_16","alias_value":"NKK32KZSHONEODUE","created_at":"2026-05-18T12:28:41.024544+00:00"},{"alias_kind":"pith_short_8","alias_value":"NKK32KZS","created_at":"2026-05-18T12:28:41.024544+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.17193","citing_title":"Proposed mixing between $2P$ and $1F$ wave charmonia","ref_index":48,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA","json":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA.json","graph_json":"https://pith.science/api/pith-number/NKK32KZSHONEODUE4PHY36YTZA/graph.json","events_json":"https://pith.science/api/pith-number/NKK32KZSHONEODUE4PHY36YTZA/events.json","paper":"https://pith.science/paper/NKK32KZS"},"agent_actions":{"view_html":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA","download_json":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA.json","view_paper":"https://pith.science/paper/NKK32KZS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.0874&json=true","fetch_graph":"https://pith.science/api/pith-number/NKK32KZSHONEODUE4PHY36YTZA/graph.json","fetch_events":"https://pith.science/api/pith-number/NKK32KZSHONEODUE4PHY36YTZA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA/action/storage_attestation","attest_author":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA/action/author_attestation","sign_citation":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA/action/citation_signature","submit_replication":"https://pith.science/pith/NKK32KZSHONEODUE4PHY36YTZA/action/replication_record"}},"created_at":"2026-05-18T01:27:46.557578+00:00","updated_at":"2026-05-18T01:27:46.557578+00:00"}