{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:IQE3GFSV2ZMSPWSMZ7QMUDNTVV","short_pith_number":"pith:IQE3GFSV","schema_version":"1.0","canonical_sha256":"4409b31655d65927da4ccfe0ca0db3ad7932a39079af01fe180678360834a5ce","source":{"kind":"arxiv","id":"1906.08353","version":3},"attestation_state":"computed","paper":{"title":"Magnetic dipole moments of the spin-$\\frac{3}{2}$ doubly heavy baryons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"U. Ozdem","submitted_at":"2019-06-19T21:01:13Z","abstract_excerpt":"The magnetic dipole moments of the spin-$\\frac{3}{2}$ doubly charmed, bottom and charmed-bottom baryons are obtained by means of the light-cone QCD sum rule. The magnetic dipole moments of these baryons encode essential knowledge of their inner structure and shape deformations. The numerical results are given as, $\\mu_{\\Xi_{cc}^{*++}} = 2.94 \\pm 0.95$, $\\mu_{\\Xi_{cc}^{*+}} = - 0.67 \\pm 0.11$, $\\mu_{\\Omega_{cc}^{*+}} =- 0.52 \\pm 0.07$, $\\mu_{\\Xi_{bb}^{*0}} = 2.30 \\pm 0.55$, $\\mu_{\\Xi_{bb}^{*-}} = -1.39 \\pm 0.32$, $\\mu_{\\Omega_{bb}^{*-}} = -1.56 \\pm 0.33$, $\\mu_{\\Xi_{bc}^{*+}} = 2.63 \\pm 0.82$, "},"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":"1906.08353","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2019-06-19T21:01:13Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"6cfd7e9d6aff034b0fd2bb36a5642aa225c745759c69feb2a955e813512b264c","abstract_canon_sha256":"7cbccc7eb7142ce901ddb32355fc6a18386af1e3e2ac70399fbc709b5134a27e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:38:45.483966Z","signature_b64":"WzgaIAoA5Wie0VGJ9a3hFRVH1DwqtbaSZ2O3D2ARUXrEcbH1lNPynewAd2V1Mx+8/dqrlXom2eGvCsjZzyALBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4409b31655d65927da4ccfe0ca0db3ad7932a39079af01fe180678360834a5ce","last_reissued_at":"2026-07-05T00:38:45.483514Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:38:45.483514Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetic dipole moments of the spin-$\\frac{3}{2}$ doubly heavy baryons","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"U. Ozdem","submitted_at":"2019-06-19T21:01:13Z","abstract_excerpt":"The magnetic dipole moments of the spin-$\\frac{3}{2}$ doubly charmed, bottom and charmed-bottom baryons are obtained by means of the light-cone QCD sum rule. The magnetic dipole moments of these baryons encode essential knowledge of their inner structure and shape deformations. The numerical results are given as, $\\mu_{\\Xi_{cc}^{*++}} = 2.94 \\pm 0.95$, $\\mu_{\\Xi_{cc}^{*+}} = - 0.67 \\pm 0.11$, $\\mu_{\\Omega_{cc}^{*+}} =- 0.52 \\pm 0.07$, $\\mu_{\\Xi_{bb}^{*0}} = 2.30 \\pm 0.55$, $\\mu_{\\Xi_{bb}^{*-}} = -1.39 \\pm 0.32$, $\\mu_{\\Omega_{bb}^{*-}} = -1.56 \\pm 0.33$, $\\mu_{\\Xi_{bc}^{*+}} = 2.63 \\pm 0.82$, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.08353","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/1906.08353/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":"1906.08353","created_at":"2026-07-05T00:38:45.483580+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.08353v3","created_at":"2026-07-05T00:38:45.483580+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.08353","created_at":"2026-07-05T00:38:45.483580+00:00"},{"alias_kind":"pith_short_12","alias_value":"IQE3GFSV2ZMS","created_at":"2026-07-05T00:38:45.483580+00:00"},{"alias_kind":"pith_short_16","alias_value":"IQE3GFSV2ZMSPWSM","created_at":"2026-07-05T00:38:45.483580+00:00"},{"alias_kind":"pith_short_8","alias_value":"IQE3GFSV","created_at":"2026-07-05T00:38:45.483580+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/IQE3GFSV2ZMSPWSMZ7QMUDNTVV","json":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV.json","graph_json":"https://pith.science/api/pith-number/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/graph.json","events_json":"https://pith.science/api/pith-number/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/events.json","paper":"https://pith.science/paper/IQE3GFSV"},"agent_actions":{"view_html":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV","download_json":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV.json","view_paper":"https://pith.science/paper/IQE3GFSV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.08353&json=true","fetch_graph":"https://pith.science/api/pith-number/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/graph.json","fetch_events":"https://pith.science/api/pith-number/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/action/storage_attestation","attest_author":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/action/author_attestation","sign_citation":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/action/citation_signature","submit_replication":"https://pith.science/pith/IQE3GFSV2ZMSPWSMZ7QMUDNTVV/action/replication_record"}},"created_at":"2026-07-05T00:38:45.483580+00:00","updated_at":"2026-07-05T00:38:45.483580+00:00"}