{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:FZXFSHFJ2V2THYH4RN32LMYGZO","short_pith_number":"pith:FZXFSHFJ","schema_version":"1.0","canonical_sha256":"2e6e591ca9d57533e0fc8b77a5b306cb9892717040b38ac1b818ef393ad06db7","source":{"kind":"arxiv","id":"1812.08021","version":2},"attestation_state":"computed","paper":{"title":"Chiral Anomaly and Schwinger Effect in Non-Abelian Gauge Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","cond-mat.mes-hall","hep-th"],"primary_cat":"hep-ph","authors_text":"Kyohei Mukaida, Ryosuke Sato, Valerie Domcke, Yohei Ema","submitted_at":"2018-12-19T15:29:55Z","abstract_excerpt":"We study the production of chiral fermions in a background of a strong non-abelian gauge field with a non-vanishing Chern-Pontryagin density. We discuss both pair production analogous to the Schwinger effect as well as asymmetric production through the chiral anomaly, sourced by the Chern-Pontryagin density. In abelian gauge theories one may nicely understand these processes by considering that the fermion dispersion relation forms discrete Landau levels. Here we extend this analysis to a non-abelian gauge theory, considering an intrinsically non-abelian isotropic and homogeneous SU(2) gauge f"},"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":"1812.08021","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-12-19T15:29:55Z","cross_cats_sorted":["astro-ph.CO","cond-mat.mes-hall","hep-th"],"title_canon_sha256":"55613e6f02de8c06349976d0ced01387b39dab3c1e82052bbf804014ffbf0dfc","abstract_canon_sha256":"2d02275176f96163d8b83ab873781310567cde18f7331bf39596e98c5e98a6d6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:44:37.855302Z","signature_b64":"ZTpJOycC49gEioC6p3fvuCt03U0CpgMONuETiOEL6awkF7Ln/jbpSQrDRzscBxUf78zLLujlQpIYbOISnpGzCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2e6e591ca9d57533e0fc8b77a5b306cb9892717040b38ac1b818ef393ad06db7","last_reissued_at":"2026-05-17T23:44:37.854821Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:44:37.854821Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral Anomaly and Schwinger Effect in Non-Abelian Gauge Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","cond-mat.mes-hall","hep-th"],"primary_cat":"hep-ph","authors_text":"Kyohei Mukaida, Ryosuke Sato, Valerie Domcke, Yohei Ema","submitted_at":"2018-12-19T15:29:55Z","abstract_excerpt":"We study the production of chiral fermions in a background of a strong non-abelian gauge field with a non-vanishing Chern-Pontryagin density. We discuss both pair production analogous to the Schwinger effect as well as asymmetric production through the chiral anomaly, sourced by the Chern-Pontryagin density. In abelian gauge theories one may nicely understand these processes by considering that the fermion dispersion relation forms discrete Landau levels. Here we extend this analysis to a non-abelian gauge theory, considering an intrinsically non-abelian isotropic and homogeneous SU(2) gauge f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.08021","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":""},"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":"1812.08021","created_at":"2026-05-17T23:44:37.854898+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.08021v2","created_at":"2026-05-17T23:44:37.854898+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.08021","created_at":"2026-05-17T23:44:37.854898+00:00"},{"alias_kind":"pith_short_12","alias_value":"FZXFSHFJ2V2T","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_16","alias_value":"FZXFSHFJ2V2THYH4","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_8","alias_value":"FZXFSHFJ","created_at":"2026-05-18T12:32:25.280505+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/FZXFSHFJ2V2THYH4RN32LMYGZO","json":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO.json","graph_json":"https://pith.science/api/pith-number/FZXFSHFJ2V2THYH4RN32LMYGZO/graph.json","events_json":"https://pith.science/api/pith-number/FZXFSHFJ2V2THYH4RN32LMYGZO/events.json","paper":"https://pith.science/paper/FZXFSHFJ"},"agent_actions":{"view_html":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO","download_json":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO.json","view_paper":"https://pith.science/paper/FZXFSHFJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.08021&json=true","fetch_graph":"https://pith.science/api/pith-number/FZXFSHFJ2V2THYH4RN32LMYGZO/graph.json","fetch_events":"https://pith.science/api/pith-number/FZXFSHFJ2V2THYH4RN32LMYGZO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO/action/storage_attestation","attest_author":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO/action/author_attestation","sign_citation":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO/action/citation_signature","submit_replication":"https://pith.science/pith/FZXFSHFJ2V2THYH4RN32LMYGZO/action/replication_record"}},"created_at":"2026-05-17T23:44:37.854898+00:00","updated_at":"2026-05-17T23:44:37.854898+00:00"}