{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:XIKK2VQD5Y6C7JYRSBDALFTF46","short_pith_number":"pith:XIKK2VQD","schema_version":"1.0","canonical_sha256":"ba14ad5603ee3c2fa7119046059665e7b67d90f1d274e64694ee32579c39db16","source":{"kind":"arxiv","id":"1611.04670","version":1},"attestation_state":"computed","paper":{"title":"Pseudoscalar condensation induced by chiral anomaly and vorticity for massive fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Jin-yi Pang, Qun Wang, Ren-hong Fang, Xin-Nian Wang","submitted_at":"2016-11-15T01:51:42Z","abstract_excerpt":"We derive the pseudoscalar condensate induced by anomaly and vorticity from the Wigner function for massive fermions in homogeneous electromagnetic fields. It has an anomaly term and a force-vorticity coupling term. As a mass effect, the pseudoscalar condensate is linearly proportional to the fermion mass in small mass expansion. By a generalization to two-flavor and three-flavor cases, the neutral pion and eta meson condensates are calculated from the Wigner function and have anomaly parts as well as force-vorticity parts, in which the anomaly part of the neutral pion condensate is consistent"},"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":"1611.04670","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-11-15T01:51:42Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4548270a9994083729cefad23727747d85ee899d15e07d6297b5a9c6172ce3bb","abstract_canon_sha256":"773aa705806e6855745f21ab37b195016c24eda04977f20e8f37610d840a5748"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:51:13.150857Z","signature_b64":"NxdGbYEM8psp5GxXbs7y3itgYMfyEdzicl8hIlkBSI4/U6DK/zzV5AOof0kNWyuFpF6kMhMi7gUjMr9Yvr4kBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba14ad5603ee3c2fa7119046059665e7b67d90f1d274e64694ee32579c39db16","last_reissued_at":"2026-05-18T00:51:13.150210Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:51:13.150210Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pseudoscalar condensation induced by chiral anomaly and vorticity for massive fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Jin-yi Pang, Qun Wang, Ren-hong Fang, Xin-Nian Wang","submitted_at":"2016-11-15T01:51:42Z","abstract_excerpt":"We derive the pseudoscalar condensate induced by anomaly and vorticity from the Wigner function for massive fermions in homogeneous electromagnetic fields. It has an anomaly term and a force-vorticity coupling term. As a mass effect, the pseudoscalar condensate is linearly proportional to the fermion mass in small mass expansion. By a generalization to two-flavor and three-flavor cases, the neutral pion and eta meson condensates are calculated from the Wigner function and have anomaly parts as well as force-vorticity parts, in which the anomaly part of the neutral pion condensate is consistent"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.04670","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":"1611.04670","created_at":"2026-05-18T00:51:13.150307+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.04670v1","created_at":"2026-05-18T00:51:13.150307+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.04670","created_at":"2026-05-18T00:51:13.150307+00:00"},{"alias_kind":"pith_short_12","alias_value":"XIKK2VQD5Y6C","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_16","alias_value":"XIKK2VQD5Y6C7JYR","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_8","alias_value":"XIKK2VQD","created_at":"2026-05-18T12:30:51.357362+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.15968","citing_title":"Anomalous Transport from Effective Field Theory","ref_index":54,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46","json":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46.json","graph_json":"https://pith.science/api/pith-number/XIKK2VQD5Y6C7JYRSBDALFTF46/graph.json","events_json":"https://pith.science/api/pith-number/XIKK2VQD5Y6C7JYRSBDALFTF46/events.json","paper":"https://pith.science/paper/XIKK2VQD"},"agent_actions":{"view_html":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46","download_json":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46.json","view_paper":"https://pith.science/paper/XIKK2VQD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.04670&json=true","fetch_graph":"https://pith.science/api/pith-number/XIKK2VQD5Y6C7JYRSBDALFTF46/graph.json","fetch_events":"https://pith.science/api/pith-number/XIKK2VQD5Y6C7JYRSBDALFTF46/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46/action/storage_attestation","attest_author":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46/action/author_attestation","sign_citation":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46/action/citation_signature","submit_replication":"https://pith.science/pith/XIKK2VQD5Y6C7JYRSBDALFTF46/action/replication_record"}},"created_at":"2026-05-18T00:51:13.150307+00:00","updated_at":"2026-05-18T00:51:13.150307+00:00"}