{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:XJDYJTSAGZNCS7NO5DJNUB42WL","short_pith_number":"pith:XJDYJTSA","schema_version":"1.0","canonical_sha256":"ba4784ce40365a297daee8d2da079ab2c2912f0ca9efe64b71e5de34e850ee95","source":{"kind":"arxiv","id":"2401.00481","version":3},"attestation_state":"computed","paper":{"title":"Analysis of the $\\mathrm{X_{AV}}$ state through its electromagnetic properties","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":"2023-12-31T12:46:42Z","abstract_excerpt":"To improve our understanding of the quark-gluon dynamics underlying multiquark states, we systematically study their electromagnetic properties. In this study, the magnetic and quadrupole moments of the theoretically predicted singly-charmed state with the quantum numbers $\\mathrm{J^P = 1^+}$ is investigated within the framework of the QCD light-cone sum rules method by considering the diquark-antidiquark configuration of this state with quark contents $[ud][\\bar{c}\\bar{s}]$. The predicted results for the magnetic and quadrupole moments are as $\\mu_{\\mathrm{X_{AV}}}=-0.89 ^{+0.14}_{-0.12}~\\mu_"},"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":"2401.00481","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-12-31T12:46:42Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"e4c5cb8d35f2621186c6762288adebca58b13d2e3d0199e63fa1b2d27fe9b57e","abstract_canon_sha256":"548a0285c25db60521afac97fdeff8ef0280075857f78b4768b0cefdd3b5f2e8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:00:40.001710Z","signature_b64":"jJU3spW4//LplASfN9WxPc1aPS/wdfGdPXZ3WoHK52wugmwzxgHYnqXUaPMDgSyPoOrSV1Zqc+p82JFrTCiaAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba4784ce40365a297daee8d2da079ab2c2912f0ca9efe64b71e5de34e850ee95","last_reissued_at":"2026-07-05T08:00:40.001083Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:00:40.001083Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analysis of the $\\mathrm{X_{AV}}$ state through its electromagnetic properties","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":"2023-12-31T12:46:42Z","abstract_excerpt":"To improve our understanding of the quark-gluon dynamics underlying multiquark states, we systematically study their electromagnetic properties. In this study, the magnetic and quadrupole moments of the theoretically predicted singly-charmed state with the quantum numbers $\\mathrm{J^P = 1^+}$ is investigated within the framework of the QCD light-cone sum rules method by considering the diquark-antidiquark configuration of this state with quark contents $[ud][\\bar{c}\\bar{s}]$. The predicted results for the magnetic and quadrupole moments are as $\\mu_{\\mathrm{X_{AV}}}=-0.89 ^{+0.14}_{-0.12}~\\mu_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.00481","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/2401.00481/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":"2401.00481","created_at":"2026-07-05T08:00:40.001159+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.00481v3","created_at":"2026-07-05T08:00:40.001159+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.00481","created_at":"2026-07-05T08:00:40.001159+00:00"},{"alias_kind":"pith_short_12","alias_value":"XJDYJTSAGZNC","created_at":"2026-07-05T08:00:40.001159+00:00"},{"alias_kind":"pith_short_16","alias_value":"XJDYJTSAGZNCS7NO","created_at":"2026-07-05T08:00:40.001159+00:00"},{"alias_kind":"pith_short_8","alias_value":"XJDYJTSA","created_at":"2026-07-05T08:00:40.001159+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/XJDYJTSAGZNCS7NO5DJNUB42WL","json":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL.json","graph_json":"https://pith.science/api/pith-number/XJDYJTSAGZNCS7NO5DJNUB42WL/graph.json","events_json":"https://pith.science/api/pith-number/XJDYJTSAGZNCS7NO5DJNUB42WL/events.json","paper":"https://pith.science/paper/XJDYJTSA"},"agent_actions":{"view_html":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL","download_json":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL.json","view_paper":"https://pith.science/paper/XJDYJTSA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.00481&json=true","fetch_graph":"https://pith.science/api/pith-number/XJDYJTSAGZNCS7NO5DJNUB42WL/graph.json","fetch_events":"https://pith.science/api/pith-number/XJDYJTSAGZNCS7NO5DJNUB42WL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL/action/storage_attestation","attest_author":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL/action/author_attestation","sign_citation":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL/action/citation_signature","submit_replication":"https://pith.science/pith/XJDYJTSAGZNCS7NO5DJNUB42WL/action/replication_record"}},"created_at":"2026-07-05T08:00:40.001159+00:00","updated_at":"2026-07-05T08:00:40.001159+00:00"}