{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:LZQWEILRBNLEQGKGIQLMYKCYDC","short_pith_number":"pith:LZQWEILR","schema_version":"1.0","canonical_sha256":"5e616221710b564819464416cc285818b18c65667a8b55264340e0202ae57043","source":{"kind":"arxiv","id":"0711.0950","version":1},"attestation_state":"computed","paper":{"title":"The effects of topological charge change in heavy ion collisions: \"Event by event P and CP violation\"","license":"","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Dmitri E. Kharzeev, Harmen J. Warringa, Larry D. McLerran","submitted_at":"2007-11-06T19:00:09Z","abstract_excerpt":"Quantum chromodynamics (QCD) contains field configurations which can be characterized by a topological invariant, the winding number Q_w. Configurations with nonzero Q_w break the charge-parity CP symmetry of QCD. We consider a novel mechanism by which these configurations can separate charge in the presence of a background magnetic field - the \"Chiral Magnetic Effect\". We argue that sufficiently large magnetic fields are created in heavy ion collisions so that the Chiral Magnetic Effect causes preferential emission of charged particles along the direction of angular momentum. Since separation"},"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":"0711.0950","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-11-06T19:00:09Z","cross_cats_sorted":["nucl-ex","nucl-th"],"title_canon_sha256":"f15809c3fc53e1e0ef8e1119048de3180390f0f8e31f8a8f293fb440549c20a2","abstract_canon_sha256":"2fbaf69cffb88772b50bdbd35cbd32d710a5474ba786e2dfd3d7b087d0ce86df"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:24:58.053258Z","signature_b64":"0x8HEJuebfkRrsgykZsAz6JPNWeDjjurbWXrjPnDmLI6gwoMK4HcqxVTCykBumfA2dYoiHxjxy3ZfA42PUkRCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e616221710b564819464416cc285818b18c65667a8b55264340e0202ae57043","last_reissued_at":"2026-07-04T17:24:58.052877Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:24:58.052877Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The effects of topological charge change in heavy ion collisions: \"Event by event P and CP violation\"","license":"","headline":"","cross_cats":["nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Dmitri E. Kharzeev, Harmen J. Warringa, Larry D. McLerran","submitted_at":"2007-11-06T19:00:09Z","abstract_excerpt":"Quantum chromodynamics (QCD) contains field configurations which can be characterized by a topological invariant, the winding number Q_w. Configurations with nonzero Q_w break the charge-parity CP symmetry of QCD. We consider a novel mechanism by which these configurations can separate charge in the presence of a background magnetic field - the \"Chiral Magnetic Effect\". We argue that sufficiently large magnetic fields are created in heavy ion collisions so that the Chiral Magnetic Effect causes preferential emission of charged particles along the direction of angular momentum. Since separation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0711.0950","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0711.0950/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"0711.0950","created_at":"2026-07-04T17:24:58.052933+00:00"},{"alias_kind":"arxiv_version","alias_value":"0711.0950v1","created_at":"2026-07-04T17:24:58.052933+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0711.0950","created_at":"2026-07-04T17:24:58.052933+00:00"},{"alias_kind":"pith_short_12","alias_value":"LZQWEILRBNLE","created_at":"2026-07-04T17:24:58.052933+00:00"},{"alias_kind":"pith_short_16","alias_value":"LZQWEILRBNLEQGKG","created_at":"2026-07-04T17:24:58.052933+00:00"},{"alias_kind":"pith_short_8","alias_value":"LZQWEILR","created_at":"2026-07-04T17:24:58.052933+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":21,"internal_anchor_count":16,"sample":[{"citing_arxiv_id":"2604.21872","citing_title":"Quark and gluon production in the presence of the time-varying chiral magnetic current","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2606.18507","citing_title":"$\\pi^0$-$\\gamma$ mixing in the presence of a strong magnetic field","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2606.28118","citing_title":"Scattering Amplitudes and Resonant Processes in QED with Chiral Chemical Potential and Chiral Magnetic Conductivity","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"2606.28111","citing_title":"Dense and Cold Magnetized Quark Matter: A Review of Magnetic-Field-Independent Regularization and the Medium Separation Scheme","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.30164","citing_title":"Isospin-Driven Splitting of Chemical Potentials in Isobar Collisions from Lattice QCD","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25487","citing_title":"A higher-harmonic observable for the chiral magnetic effect in heavy-ion collisions","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"1907.03990","citing_title":"Effect of anomalous magnetic moment of quarks on the phase structure and mesonic properties in the NJL model","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"1907.04486","citing_title":"Critical behaviour of an effective relativistic mean field model in the presence of magnetic background and boundaries","ref_index":19,"is_internal_anchor":true},{"citing_arxiv_id":"2006.00200","citing_title":"Analysis of the QCD Kondo phase using random matrices","ref_index":83,"is_internal_anchor":true},{"citing_arxiv_id":"2601.18354","citing_title":"Chiral Properties of $(2\\!+\\!1)$-Flavor QCD in Magnetic Fields at Zero Temperature","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19012","citing_title":"Meson Octet in a Uniform Magnetic Field","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2508.17757","citing_title":"Stationary States for Fermions in an External Electric Field","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2510.17597","citing_title":"Photon radiation induced by rescattering in strong-interacting medium with a magnetic field","ref_index":40,"is_internal_anchor":true},{"citing_arxiv_id":"2511.19255","citing_title":"Magnetic susceptibility of a hot hadronic medium and quark degrees of freedom near the QCD cross-over point","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2601.22422","citing_title":"Spectral function for pions in magnetic field","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2605.12554","citing_title":"Spin dynamics and polarization in relativistic systems: recent developments","ref_index":191,"is_internal_anchor":true},{"citing_arxiv_id":"2604.27800","citing_title":"Electromagnetic response of a relativistic drifting plasma","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21872","citing_title":"Quark and gluon production in the presence of the time-varying chiral magnetic current","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2604.06248","citing_title":"Relativistic Barnett effect and Curie law in a rigidly rotating free Fermi gas","ref_index":10,"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":6,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15897","citing_title":"Delineating neutral and charged mesons in magnetic fields","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC","json":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC.json","graph_json":"https://pith.science/api/pith-number/LZQWEILRBNLEQGKGIQLMYKCYDC/graph.json","events_json":"https://pith.science/api/pith-number/LZQWEILRBNLEQGKGIQLMYKCYDC/events.json","paper":"https://pith.science/paper/LZQWEILR"},"agent_actions":{"view_html":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC","download_json":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC.json","view_paper":"https://pith.science/paper/LZQWEILR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0711.0950&json=true","fetch_graph":"https://pith.science/api/pith-number/LZQWEILRBNLEQGKGIQLMYKCYDC/graph.json","fetch_events":"https://pith.science/api/pith-number/LZQWEILRBNLEQGKGIQLMYKCYDC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC/action/storage_attestation","attest_author":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC/action/author_attestation","sign_citation":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC/action/citation_signature","submit_replication":"https://pith.science/pith/LZQWEILRBNLEQGKGIQLMYKCYDC/action/replication_record"}},"created_at":"2026-07-04T17:24:58.052933+00:00","updated_at":"2026-07-04T17:24:58.052933+00:00"}