{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:SWVNI7PP64AY7S7NHWT42UJRD6","short_pith_number":"pith:SWVNI7PP","schema_version":"1.0","canonical_sha256":"95aad47deff7018fcbed3da7cd51311f85b8ecb40fd447d3165f9ef269cc9ac5","source":{"kind":"arxiv","id":"1410.6388","version":1},"attestation_state":"computed","paper":{"title":"Finite temperature quark-gluon vertex with a magnetic field in the Hard Thermal Loop approximation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alejandro Ayala, J.J. Cobos-Martinez, Maria Elena Tejeda-Yeomans, M. Loewe, R. Zamora","submitted_at":"2014-10-23T15:06:13Z","abstract_excerpt":"We compute the thermo-magnetic correction to the quark-gluon vertex in the presence of a weak magnetic field within the Hard Thermal Loop approximation. The vertex satisfies a QED-like Ward identity with the quark self-energy. The only vertex components that get modified are the longitudinal ones. The calculation provides a first principles result for the quark anomalous magnetic moment at high temperature in a weak magnetic field. We extract the effective thermo-magnetic quark-gluon coupling and show that this decreases as a function of the field strength. The result supports the idea that th"},"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":"1410.6388","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-10-23T15:06:13Z","cross_cats_sorted":["hep-lat","hep-th","nucl-th"],"title_canon_sha256":"b4681076423f55c69504d8a7b6d0a2f786ca54d61cc11726cae292c9a94b12a4","abstract_canon_sha256":"ef5b5e3a271d8871bb04e980236befd7fd12ee6936a2ef21604681e68b09e2b0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:40.495530Z","signature_b64":"ju47dDMnAeXpUBKfSMPWldvJqBRT33wB9yI+DZYBN4xbsxplYcpIVBSFqa8PAUv5CN+kP4unVvZ1DeAOpc57Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"95aad47deff7018fcbed3da7cd51311f85b8ecb40fd447d3165f9ef269cc9ac5","last_reissued_at":"2026-05-18T01:41:40.494981Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:40.494981Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite temperature quark-gluon vertex with a magnetic field in the Hard Thermal Loop approximation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"Alejandro Ayala, J.J. Cobos-Martinez, Maria Elena Tejeda-Yeomans, M. Loewe, R. Zamora","submitted_at":"2014-10-23T15:06:13Z","abstract_excerpt":"We compute the thermo-magnetic correction to the quark-gluon vertex in the presence of a weak magnetic field within the Hard Thermal Loop approximation. The vertex satisfies a QED-like Ward identity with the quark self-energy. The only vertex components that get modified are the longitudinal ones. The calculation provides a first principles result for the quark anomalous magnetic moment at high temperature in a weak magnetic field. We extract the effective thermo-magnetic quark-gluon coupling and show that this decreases as a function of the field strength. The result supports the idea that th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.6388","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":""},"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":"1410.6388","created_at":"2026-05-18T01:41:40.495054+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.6388v1","created_at":"2026-05-18T01:41:40.495054+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.6388","created_at":"2026-05-18T01:41:40.495054+00:00"},{"alias_kind":"pith_short_12","alias_value":"SWVNI7PP64AY","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"SWVNI7PP64AY7S7N","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"SWVNI7PP","created_at":"2026-05-18T12:28:49.207871+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/SWVNI7PP64AY7S7NHWT42UJRD6","json":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6.json","graph_json":"https://pith.science/api/pith-number/SWVNI7PP64AY7S7NHWT42UJRD6/graph.json","events_json":"https://pith.science/api/pith-number/SWVNI7PP64AY7S7NHWT42UJRD6/events.json","paper":"https://pith.science/paper/SWVNI7PP"},"agent_actions":{"view_html":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6","download_json":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6.json","view_paper":"https://pith.science/paper/SWVNI7PP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.6388&json=true","fetch_graph":"https://pith.science/api/pith-number/SWVNI7PP64AY7S7NHWT42UJRD6/graph.json","fetch_events":"https://pith.science/api/pith-number/SWVNI7PP64AY7S7NHWT42UJRD6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6/action/storage_attestation","attest_author":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6/action/author_attestation","sign_citation":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6/action/citation_signature","submit_replication":"https://pith.science/pith/SWVNI7PP64AY7S7NHWT42UJRD6/action/replication_record"}},"created_at":"2026-05-18T01:41:40.495054+00:00","updated_at":"2026-05-18T01:41:40.495054+00:00"}