{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:L2XCK27GU52FZPDNDODMIX4DGL","short_pith_number":"pith:L2XCK27G","schema_version":"1.0","canonical_sha256":"5eae256be6a7745cbc6d1b86c45f8332db86faf839c20d4c3ec49f5a79a65449","source":{"kind":"arxiv","id":"hep-ph/0406125","version":2},"attestation_state":"computed","paper":{"title":"Parity violation in hot QCD: why it can happen, and how to look for it","license":"","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"D. Kharzeev","submitted_at":"2004-06-10T18:02:43Z","abstract_excerpt":"The arguments for the possibility of violation of P and CP symmetries of strong interactions at finite temperature are presented. A new way of observing these effects in heavy ion collisions is proposed -- it is shown that parity violation should manifest itself in the asymmetry between positive and negative pions with respect to the reaction plane. Basing on topological considerations, we derive a {\\it lower} bound on the magnitude of the expected asymmetry, which may appear within the reach of the current and/or future heavy ion experiments."},"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":"hep-ph/0406125","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-06-10T18:02:43Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"2245ab3428c10ba86f14ca03aab3345e1de7cf50e739d1705915d8e16d2de8b8","abstract_canon_sha256":"b2c6d82750c437471ebcc3366e16e7eebe733dff4832ff614139f69663b0c85e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:22:51.970679Z","signature_b64":"svDsT0uYk9dDjCbWWj+/z1tD35XSIzyq72Lp+SWJoSUhEtssnOJJMmtxtHEZljd3gRdNglr+n8lFOV2xFxDlBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5eae256be6a7745cbc6d1b86c45f8332db86faf839c20d4c3ec49f5a79a65449","last_reissued_at":"2026-05-18T04:22:51.970230Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:22:51.970230Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Parity violation in hot QCD: why it can happen, and how to look for it","license":"","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"D. Kharzeev","submitted_at":"2004-06-10T18:02:43Z","abstract_excerpt":"The arguments for the possibility of violation of P and CP symmetries of strong interactions at finite temperature are presented. A new way of observing these effects in heavy ion collisions is proposed -- it is shown that parity violation should manifest itself in the asymmetry between positive and negative pions with respect to the reaction plane. Basing on topological considerations, we derive a {\\it lower} bound on the magnitude of the expected asymmetry, which may appear within the reach of the current and/or future heavy ion experiments."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0406125","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":"hep-ph/0406125","created_at":"2026-05-18T04:22:51.970296+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0406125v2","created_at":"2026-05-18T04:22:51.970296+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0406125","created_at":"2026-05-18T04:22:51.970296+00:00"},{"alias_kind":"pith_short_12","alias_value":"L2XCK27GU52F","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_16","alias_value":"L2XCK27GU52FZPDN","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_8","alias_value":"L2XCK27G","created_at":"2026-05-18T12:25:52.687210+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.23125","citing_title":"Quark orbital angular momentum as a chiral magnetic effect","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2604.21872","citing_title":"Quark and gluon production in the presence of the time-varying chiral magnetic current","ref_index":6,"is_internal_anchor":false},{"citing_arxiv_id":"2604.05654","citing_title":"Probing the chiral magnetic effect via transverse spherocity event classification in relativistic heavy-ion collisions","ref_index":31,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL","json":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL.json","graph_json":"https://pith.science/api/pith-number/L2XCK27GU52FZPDNDODMIX4DGL/graph.json","events_json":"https://pith.science/api/pith-number/L2XCK27GU52FZPDNDODMIX4DGL/events.json","paper":"https://pith.science/paper/L2XCK27G"},"agent_actions":{"view_html":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL","download_json":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL.json","view_paper":"https://pith.science/paper/L2XCK27G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0406125&json=true","fetch_graph":"https://pith.science/api/pith-number/L2XCK27GU52FZPDNDODMIX4DGL/graph.json","fetch_events":"https://pith.science/api/pith-number/L2XCK27GU52FZPDNDODMIX4DGL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL/action/storage_attestation","attest_author":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL/action/author_attestation","sign_citation":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL/action/citation_signature","submit_replication":"https://pith.science/pith/L2XCK27GU52FZPDNDODMIX4DGL/action/replication_record"}},"created_at":"2026-05-18T04:22:51.970296+00:00","updated_at":"2026-05-18T04:22:51.970296+00:00"}