{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:ANGXQSRMGFJDVRXKA5HQZVYNLA","short_pith_number":"pith:ANGXQSRM","schema_version":"1.0","canonical_sha256":"034d784a2c31523ac6ea074f0cd70d58086a15a4cd2d2bc3c6cba393c4ca41c8","source":{"kind":"arxiv","id":"2108.01840","version":1},"attestation_state":"computed","paper":{"title":"Radiative M1 transitions of heavy baryons: Effective Quark Mass Scheme","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Avijit Hazra, Rohit Dhir, Saheli Rakshit","submitted_at":"2021-08-04T04:27:06Z","abstract_excerpt":"We calculate the magnetic moments of ground state $J^P=\\frac{1}{2}^+$ and $J^P=\\frac{3}{2}^+$ heavy flavor charm and bottom baryon states employing the concept of effective mass based on single gluon exchange interaction coupling to the spectator quarks in the non-relativistic quark model. We exploit the current experimental information in the heavy flavor sector to estimate the interaction contributions to get the effective masses of the quarks inside the baryons. We study the spin $\\frac{1}{2}^{'+} \\rightarrow \\frac{1}{2}^+$, $\\frac{3}{2}^+ \\rightarrow \\frac{1}{2}^+$, and $\\frac{3}{2}^+ \\rig"},"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":"2108.01840","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-08-04T04:27:06Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"1b71e0c55b33d88d91fb41b590d026b2ac186f4d0484ade72f41d787f81e8aec","abstract_canon_sha256":"9b48a3a0ad250e7c01e65f2d3b6e101e8c19df4ad331d23b8fbed75ed6aef849"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:14:24.979739Z","signature_b64":"QJ7OeWp+QESvBYVlN8wT1Xw16hBVwSOnZdl3wywhi3S44oNEusJYxtky98lU97BQbUwH6DNH8v2wbLQCFHNTAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"034d784a2c31523ac6ea074f0cd70d58086a15a4cd2d2bc3c6cba393c4ca41c8","last_reissued_at":"2026-07-05T03:14:24.979327Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:14:24.979327Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative M1 transitions of heavy baryons: Effective Quark Mass Scheme","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Avijit Hazra, Rohit Dhir, Saheli Rakshit","submitted_at":"2021-08-04T04:27:06Z","abstract_excerpt":"We calculate the magnetic moments of ground state $J^P=\\frac{1}{2}^+$ and $J^P=\\frac{3}{2}^+$ heavy flavor charm and bottom baryon states employing the concept of effective mass based on single gluon exchange interaction coupling to the spectator quarks in the non-relativistic quark model. We exploit the current experimental information in the heavy flavor sector to estimate the interaction contributions to get the effective masses of the quarks inside the baryons. We study the spin $\\frac{1}{2}^{'+} \\rightarrow \\frac{1}{2}^+$, $\\frac{3}{2}^+ \\rightarrow \\frac{1}{2}^+$, and $\\frac{3}{2}^+ \\rig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2108.01840","kind":"arxiv","version":1},"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/2108.01840/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":"2108.01840","created_at":"2026-07-05T03:14:24.979383+00:00"},{"alias_kind":"arxiv_version","alias_value":"2108.01840v1","created_at":"2026-07-05T03:14:24.979383+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2108.01840","created_at":"2026-07-05T03:14:24.979383+00:00"},{"alias_kind":"pith_short_12","alias_value":"ANGXQSRMGFJD","created_at":"2026-07-05T03:14:24.979383+00:00"},{"alias_kind":"pith_short_16","alias_value":"ANGXQSRMGFJDVRXK","created_at":"2026-07-05T03:14:24.979383+00:00"},{"alias_kind":"pith_short_8","alias_value":"ANGXQSRM","created_at":"2026-07-05T03:14:24.979383+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.18796","citing_title":"Mass spectrum, magnetic moments and Regge trajectories of $\\Omega_{ccb}$ and $\\Omega_{cbb}$ baryons in the nonrelativistic quark--diquark model","ref_index":94,"is_internal_anchor":true},{"citing_arxiv_id":"2603.01037","citing_title":"Quark-diquark effective mass formalism for heavy baryon spectroscopy","ref_index":93,"is_internal_anchor":false},{"citing_arxiv_id":"2604.18796","citing_title":"Mass spectrum, magnetic moments and Regge trajectories of $\\Omega_{ccb}$ and $\\Omega_{cbb}$ baryons in the nonrelativistic quark--diquark model","ref_index":94,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA","json":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA.json","graph_json":"https://pith.science/api/pith-number/ANGXQSRMGFJDVRXKA5HQZVYNLA/graph.json","events_json":"https://pith.science/api/pith-number/ANGXQSRMGFJDVRXKA5HQZVYNLA/events.json","paper":"https://pith.science/paper/ANGXQSRM"},"agent_actions":{"view_html":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA","download_json":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA.json","view_paper":"https://pith.science/paper/ANGXQSRM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2108.01840&json=true","fetch_graph":"https://pith.science/api/pith-number/ANGXQSRMGFJDVRXKA5HQZVYNLA/graph.json","fetch_events":"https://pith.science/api/pith-number/ANGXQSRMGFJDVRXKA5HQZVYNLA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA/action/storage_attestation","attest_author":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA/action/author_attestation","sign_citation":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA/action/citation_signature","submit_replication":"https://pith.science/pith/ANGXQSRMGFJDVRXKA5HQZVYNLA/action/replication_record"}},"created_at":"2026-07-05T03:14:24.979383+00:00","updated_at":"2026-07-05T03:14:24.979383+00:00"}