{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:WJRFPVWQSIGJJNUWDA3SMEOYDX","short_pith_number":"pith:WJRFPVWQ","schema_version":"1.0","canonical_sha256":"b26257d6d0920c94b69618372611d81dfdd7e296b7814cbdff8c02ac5646bb8d","source":{"kind":"arxiv","id":"2104.14112","version":2},"attestation_state":"computed","paper":{"title":"Thermomagnetic modification of the anomalous magnetic moment of quarks using the NJL model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Nilanjan Chaudhuri, Pradip Roy, Snigdha Ghosh, Sourav Sarkar","submitted_at":"2021-04-29T05:10:12Z","abstract_excerpt":"The effective photon-quark-antiquark ($\\gamma q \\overline{q}$) vertex function is evaluated at finite temperature in the presence of an arbitrary external magnetic field using the two-flavor gauged Nambu--Jona-Lasinio (NJL) model in the mean field approximation. The lowest order diagram contributing to the magnetic form factor and the anomalous magnetic moment (AMM) of the quarks is calculated at finite temperature and external magnetic field using the imaginary time formalism of finite temperature field theory and the Schwinger proper time formalism. The Schwinger propagator including all the"},"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":"2104.14112","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-04-29T05:10:12Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"b8d82fc7edecdc0f2a5ae69fb82eb872b3c30a1e6c8b4481d99bd4907874378f","abstract_canon_sha256":"119f5a8afe78528b58c22cce476f83ed8a91c0a53d1b1d42bbac4ce289bb69b8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:49:30.227577Z","signature_b64":"yqZp+xRRMLvSysGSkxyWk3S1iyuau+0MJ+oNyY5Id20t0nKMm3nlou70ZBOfSJTjAjvR6t3fl986Glwec4cbDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b26257d6d0920c94b69618372611d81dfdd7e296b7814cbdff8c02ac5646bb8d","last_reissued_at":"2026-07-05T02:49:30.227143Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:49:30.227143Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermomagnetic modification of the anomalous magnetic moment of quarks using the NJL model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Nilanjan Chaudhuri, Pradip Roy, Snigdha Ghosh, Sourav Sarkar","submitted_at":"2021-04-29T05:10:12Z","abstract_excerpt":"The effective photon-quark-antiquark ($\\gamma q \\overline{q}$) vertex function is evaluated at finite temperature in the presence of an arbitrary external magnetic field using the two-flavor gauged Nambu--Jona-Lasinio (NJL) model in the mean field approximation. The lowest order diagram contributing to the magnetic form factor and the anomalous magnetic moment (AMM) of the quarks is calculated at finite temperature and external magnetic field using the imaginary time formalism of finite temperature field theory and the Schwinger proper time formalism. The Schwinger propagator including all the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2104.14112","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/2104.14112/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":"2104.14112","created_at":"2026-07-05T02:49:30.227195+00:00"},{"alias_kind":"arxiv_version","alias_value":"2104.14112v2","created_at":"2026-07-05T02:49:30.227195+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2104.14112","created_at":"2026-07-05T02:49:30.227195+00:00"},{"alias_kind":"pith_short_12","alias_value":"WJRFPVWQSIGJ","created_at":"2026-07-05T02:49:30.227195+00:00"},{"alias_kind":"pith_short_16","alias_value":"WJRFPVWQSIGJJNUW","created_at":"2026-07-05T02:49:30.227195+00:00"},{"alias_kind":"pith_short_8","alias_value":"WJRFPVWQ","created_at":"2026-07-05T02:49:30.227195+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2511.19255","citing_title":"Magnetic susceptibility of a hot hadronic medium and quark degrees of freedom near the QCD cross-over point","ref_index":83,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX","json":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX.json","graph_json":"https://pith.science/api/pith-number/WJRFPVWQSIGJJNUWDA3SMEOYDX/graph.json","events_json":"https://pith.science/api/pith-number/WJRFPVWQSIGJJNUWDA3SMEOYDX/events.json","paper":"https://pith.science/paper/WJRFPVWQ"},"agent_actions":{"view_html":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX","download_json":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX.json","view_paper":"https://pith.science/paper/WJRFPVWQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2104.14112&json=true","fetch_graph":"https://pith.science/api/pith-number/WJRFPVWQSIGJJNUWDA3SMEOYDX/graph.json","fetch_events":"https://pith.science/api/pith-number/WJRFPVWQSIGJJNUWDA3SMEOYDX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX/action/storage_attestation","attest_author":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX/action/author_attestation","sign_citation":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX/action/citation_signature","submit_replication":"https://pith.science/pith/WJRFPVWQSIGJJNUWDA3SMEOYDX/action/replication_record"}},"created_at":"2026-07-05T02:49:30.227195+00:00","updated_at":"2026-07-05T02:49:30.227195+00:00"}