{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:42QPZTMYYJDNHLHMDSVANDYZRO","short_pith_number":"pith:42QPZTMY","schema_version":"1.0","canonical_sha256":"e6a0fccd98c246d3acec1caa068f198babf8655bc38dee359b9b491cf8abdcfb","source":{"kind":"arxiv","id":"1704.05887","version":2},"attestation_state":"computed","paper":{"title":"Simulating chiral magnetic effect and anomalous transport phenomena in the pre-equilibrium stages of heavy-ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Mark Mace, Niklas Mueller, Sayantan Sharma, Soeren Schlichting","submitted_at":"2017-04-13T08:06:21Z","abstract_excerpt":"We present a first principles approach to study the Chiral Magnetic Effect during the pre-equilibrium stage of a heavy-ion collision. We discuss the dynamics of the Chiral Magnetic Effect and Chiral Magnetic Wave based on real-time lattice simulations with dynamical (Wilson and Overlap) fermions simultaneously coupled to color and electromagnetic fields. While for light quarks we observe a dissipation-less transport of charges as in anomalous hydrodynamics, we demonstrate that for heavier quarks the effects of explicit chiral symmetry breaking lead to a significant reduction of the associated "},"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":"1704.05887","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-04-13T08:06:21Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"27126efda291cb7fa8cefc5ed306d8d724619703cbb79fe54298ad653f9c36bd","abstract_canon_sha256":"517835b9f034cf9b62c44c555a08e377893aa12f66e032cb6bbfe33c454f068d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:28.316076Z","signature_b64":"WVfI6LnC7he3f9jP3bwGwQcylGKAN7fikfDUV+Nsh1lQd/yVUGx4xvnBh+IS6dLO+edEqA363sbBxcd+ScPaBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6a0fccd98c246d3acec1caa068f198babf8655bc38dee359b9b491cf8abdcfb","last_reissued_at":"2026-05-18T00:21:28.315464Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:28.315464Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Simulating chiral magnetic effect and anomalous transport phenomena in the pre-equilibrium stages of heavy-ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Mark Mace, Niklas Mueller, Sayantan Sharma, Soeren Schlichting","submitted_at":"2017-04-13T08:06:21Z","abstract_excerpt":"We present a first principles approach to study the Chiral Magnetic Effect during the pre-equilibrium stage of a heavy-ion collision. We discuss the dynamics of the Chiral Magnetic Effect and Chiral Magnetic Wave based on real-time lattice simulations with dynamical (Wilson and Overlap) fermions simultaneously coupled to color and electromagnetic fields. While for light quarks we observe a dissipation-less transport of charges as in anomalous hydrodynamics, we demonstrate that for heavier quarks the effects of explicit chiral symmetry breaking lead to a significant reduction of the associated "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.05887","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":"1704.05887","created_at":"2026-05-18T00:21:28.315570+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.05887v2","created_at":"2026-05-18T00:21:28.315570+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.05887","created_at":"2026-05-18T00:21:28.315570+00:00"},{"alias_kind":"pith_short_12","alias_value":"42QPZTMYYJDN","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_16","alias_value":"42QPZTMYYJDNHLHM","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_8","alias_value":"42QPZTMY","created_at":"2026-05-18T12:30:58.224056+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/42QPZTMYYJDNHLHMDSVANDYZRO","json":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO.json","graph_json":"https://pith.science/api/pith-number/42QPZTMYYJDNHLHMDSVANDYZRO/graph.json","events_json":"https://pith.science/api/pith-number/42QPZTMYYJDNHLHMDSVANDYZRO/events.json","paper":"https://pith.science/paper/42QPZTMY"},"agent_actions":{"view_html":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO","download_json":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO.json","view_paper":"https://pith.science/paper/42QPZTMY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.05887&json=true","fetch_graph":"https://pith.science/api/pith-number/42QPZTMYYJDNHLHMDSVANDYZRO/graph.json","fetch_events":"https://pith.science/api/pith-number/42QPZTMYYJDNHLHMDSVANDYZRO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO/action/storage_attestation","attest_author":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO/action/author_attestation","sign_citation":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO/action/citation_signature","submit_replication":"https://pith.science/pith/42QPZTMYYJDNHLHMDSVANDYZRO/action/replication_record"}},"created_at":"2026-05-18T00:21:28.315570+00:00","updated_at":"2026-05-18T00:21:28.315570+00:00"}