{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:B3LU5NS2IJ3FHSBEUD6P7BHRTL","short_pith_number":"pith:B3LU5NS2","schema_version":"1.0","canonical_sha256":"0ed74eb65a427653c824a0fcff84f19af2f411f4c036d762d77abce6dd37f016","source":{"kind":"arxiv","id":"hep-ex/0310050","version":2},"attestation_state":"computed","paper":{"title":"Observation of a Narrow Meson Decaying to Ds pi0 gamma at a Mass of 2.458 GeV/c^2","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, the BABAR Collaboration: B. Aubert","submitted_at":"2003-10-24T15:26:57Z","abstract_excerpt":"A narrow state, which we label DsJ(2458)+, with mass 2458.0 +/- 1.0(stat.) +/- 1.0(syst.) MeV/c^2, is observed in the inclusive Ds+ pi0 \\gamma$ mass distribution in 91 fb-1 of e^+e^- annihilation data recorded by the BABAR detector at the PEP-II asymmetric-energy e^+e^- storage ring. The observed width is consistent with the experimental resolution. The data favor decay through Ds*(2112)+ pi0 rather than through DsJ*(2317)+ gamma. An analysis of Ds+ pi0 data accounting for the influence of the DsJ(2458)+ produces a DsJ*(2317)+ mass of 2317.3 +/- 0.4(stat.) +/- 0.8(syst.) MeV/c^2."},"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-ex/0310050","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2003-10-24T15:26:57Z","cross_cats_sorted":[],"title_canon_sha256":"637e530e6e39d9783c6f18700f5edd5915259f2e7310339c9fe0a74fcc3e1593","abstract_canon_sha256":"c1854ce423b707081ffd14c51f0860b566156a2bceb3aa6210fdc3e584a9979e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:32:14.468564Z","signature_b64":"cmns8Uy06htXo8vYRhTveTcGzALo6zjEQRy1Yy/PukYItxzTC/eGjVbaxKY9D7ZPPDq7wLY/lZVFzsyDdNd3Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ed74eb65a427653c824a0fcff84f19af2f411f4c036d762d77abce6dd37f016","last_reissued_at":"2026-07-04T15:32:14.468155Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:32:14.468155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Observation of a Narrow Meson Decaying to Ds pi0 gamma at a Mass of 2.458 GeV/c^2","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, the BABAR Collaboration: B. Aubert","submitted_at":"2003-10-24T15:26:57Z","abstract_excerpt":"A narrow state, which we label DsJ(2458)+, with mass 2458.0 +/- 1.0(stat.) +/- 1.0(syst.) MeV/c^2, is observed in the inclusive Ds+ pi0 \\gamma$ mass distribution in 91 fb-1 of e^+e^- annihilation data recorded by the BABAR detector at the PEP-II asymmetric-energy e^+e^- storage ring. The observed width is consistent with the experimental resolution. The data favor decay through Ds*(2112)+ pi0 rather than through DsJ*(2317)+ gamma. An analysis of Ds+ pi0 data accounting for the influence of the DsJ(2458)+ produces a DsJ*(2317)+ mass of 2317.3 +/- 0.4(stat.) +/- 0.8(syst.) MeV/c^2."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0310050","kind":"arxiv","version":2},"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-ex/0310050/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-ex/0310050","created_at":"2026-07-04T15:32:14.468217+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0310050v2","created_at":"2026-07-04T15:32:14.468217+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0310050","created_at":"2026-07-04T15:32:14.468217+00:00"},{"alias_kind":"pith_short_12","alias_value":"B3LU5NS2IJ3F","created_at":"2026-07-04T15:32:14.468217+00:00"},{"alias_kind":"pith_short_16","alias_value":"B3LU5NS2IJ3FHSBE","created_at":"2026-07-04T15:32:14.468217+00:00"},{"alias_kind":"pith_short_8","alias_value":"B3LU5NS2","created_at":"2026-07-04T15:32:14.468217+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"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":6,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL","json":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL.json","graph_json":"https://pith.science/api/pith-number/B3LU5NS2IJ3FHSBEUD6P7BHRTL/graph.json","events_json":"https://pith.science/api/pith-number/B3LU5NS2IJ3FHSBEUD6P7BHRTL/events.json","paper":"https://pith.science/paper/B3LU5NS2"},"agent_actions":{"view_html":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL","download_json":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL.json","view_paper":"https://pith.science/paper/B3LU5NS2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0310050&json=true","fetch_graph":"https://pith.science/api/pith-number/B3LU5NS2IJ3FHSBEUD6P7BHRTL/graph.json","fetch_events":"https://pith.science/api/pith-number/B3LU5NS2IJ3FHSBEUD6P7BHRTL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL/action/storage_attestation","attest_author":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL/action/author_attestation","sign_citation":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL/action/citation_signature","submit_replication":"https://pith.science/pith/B3LU5NS2IJ3FHSBEUD6P7BHRTL/action/replication_record"}},"created_at":"2026-07-04T15:32:14.468217+00:00","updated_at":"2026-07-04T15:32:14.468217+00:00"}