{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:V6OBA2BOVCRCAB7BE52C5T2EFD","short_pith_number":"pith:V6OBA2BO","schema_version":"1.0","canonical_sha256":"af9c10682ea8a22007e127742ecf4428ea43fcc08ea9f5f6286334265e225689","source":{"kind":"arxiv","id":"1206.3128","version":2},"attestation_state":"computed","paper":{"title":"Wess-Zumino-Witten action and photons from the Chiral Magnetic Effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kazuya Mameda, Kenji Fukushima","submitted_at":"2012-06-14T14:59:24Z","abstract_excerpt":"We revisit the Chiral Magnetic Effect (CME) using the chiral Lagrangian. We demonstrate that the electric-current formula of the CME is derived immediately from the contact part of the Wess-Zumino-Witten action. This implies that the CME could be, if observed, a signature for the local parity violation, but a direct evidence for neither quark deconfinement nor chiral restoration. We also discuss the reverse Chiral Magnetic Primakoff Effect, i.e. the real photon production through the vertex associated with the CME, which is kinematically possible for space-time inhomogeneous configurations of "},"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":"1206.3128","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-06-14T14:59:24Z","cross_cats_sorted":[],"title_canon_sha256":"f622211994940f4a13c6d0e226ca74f447c86addb78b8397d0f19cdc59f22d3c","abstract_canon_sha256":"5f5e89f7886883e8d4da4da6a619ce02f7a3dd383c1c1332e90883455ae94a65"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:58.683545Z","signature_b64":"UruqEqy0xPYIZ+5dNQyb2Vsr+t7CdV80t2iq5h1rQVHwXvZwIpMJSr4XAaFr4LI2eeAs2DGBvQRiRrG40wxRAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af9c10682ea8a22007e127742ecf4428ea43fcc08ea9f5f6286334265e225689","last_reissued_at":"2026-05-18T01:56:58.683092Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:58.683092Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wess-Zumino-Witten action and photons from the Chiral Magnetic Effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kazuya Mameda, Kenji Fukushima","submitted_at":"2012-06-14T14:59:24Z","abstract_excerpt":"We revisit the Chiral Magnetic Effect (CME) using the chiral Lagrangian. We demonstrate that the electric-current formula of the CME is derived immediately from the contact part of the Wess-Zumino-Witten action. This implies that the CME could be, if observed, a signature for the local parity violation, but a direct evidence for neither quark deconfinement nor chiral restoration. We also discuss the reverse Chiral Magnetic Primakoff Effect, i.e. the real photon production through the vertex associated with the CME, which is kinematically possible for space-time inhomogeneous configurations of "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.3128","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":"1206.3128","created_at":"2026-05-18T01:56:58.683161+00:00"},{"alias_kind":"arxiv_version","alias_value":"1206.3128v2","created_at":"2026-05-18T01:56:58.683161+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.3128","created_at":"2026-05-18T01:56:58.683161+00:00"},{"alias_kind":"pith_short_12","alias_value":"V6OBA2BOVCRC","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_16","alias_value":"V6OBA2BOVCRCAB7B","created_at":"2026-05-18T12:27:25.539911+00:00"},{"alias_kind":"pith_short_8","alias_value":"V6OBA2BO","created_at":"2026-05-18T12:27:25.539911+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.12923","citing_title":"Polarized electromagnetic radiation by chiral media with time-dependent chiral chemical potential","ref_index":4,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD","json":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD.json","graph_json":"https://pith.science/api/pith-number/V6OBA2BOVCRCAB7BE52C5T2EFD/graph.json","events_json":"https://pith.science/api/pith-number/V6OBA2BOVCRCAB7BE52C5T2EFD/events.json","paper":"https://pith.science/paper/V6OBA2BO"},"agent_actions":{"view_html":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD","download_json":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD.json","view_paper":"https://pith.science/paper/V6OBA2BO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1206.3128&json=true","fetch_graph":"https://pith.science/api/pith-number/V6OBA2BOVCRCAB7BE52C5T2EFD/graph.json","fetch_events":"https://pith.science/api/pith-number/V6OBA2BOVCRCAB7BE52C5T2EFD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD/action/storage_attestation","attest_author":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD/action/author_attestation","sign_citation":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD/action/citation_signature","submit_replication":"https://pith.science/pith/V6OBA2BOVCRCAB7BE52C5T2EFD/action/replication_record"}},"created_at":"2026-05-18T01:56:58.683161+00:00","updated_at":"2026-05-18T01:56:58.683161+00:00"}