{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:D7Z2LJ3UDNLFWQPDDXIYRJ5ME2","short_pith_number":"pith:D7Z2LJ3U","schema_version":"1.0","canonical_sha256":"1ff3a5a7741b565b41e31dd188a7ac2696ec12394fc6a12e82297075ed778ef4","source":{"kind":"arxiv","id":"1505.04582","version":3},"attestation_state":"computed","paper":{"title":"Chiral magnetic conductivity in an interacting lattice model of parity-breaking Weyl semimetal","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"M. Puhr, P. V. Buividovich, S. N. Valgushev","submitted_at":"2015-05-18T10:24:46Z","abstract_excerpt":"We report on the mean-field study of the Chiral Magnetic Effect (CME) in static magnetic fields within a simple model of a parity-breaking Weyl semimetal given by the lattice Wilson-Dirac Hamiltonian with constant chiral chemical potential. We consider both the mean-field renormalization of the model parameters and nontrivial corrections to the CME originating from re-summed ladder diagrams with arbitrary number of loops. We find that on-site repulsive interactions affect the chiral magnetic conductivity almost exclusively through the enhancement of the renormalized chiral chemical potential. "},"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":"1505.04582","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-05-18T10:24:46Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"40fdba62988baaa6d53cdb2943f0c03fb306ad28358c9249f48b34451bb8d21f","abstract_canon_sha256":"d0e6b1d39190081b82488ef69fe0cc894afbe9ce4d4255cf20999c04b13e9ec1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:25:18.120715Z","signature_b64":"BqZpuO17yxt6RjmfSOeC/9/Pg34ZW2iJYvbrZW11yMuLt9OTnDavLL7lXRNNIAoM2uSNC7cT+N32LichK3LBAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1ff3a5a7741b565b41e31dd188a7ac2696ec12394fc6a12e82297075ed778ef4","last_reissued_at":"2026-05-18T01:25:18.120007Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:25:18.120007Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral magnetic conductivity in an interacting lattice model of parity-breaking Weyl semimetal","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"M. Puhr, P. V. Buividovich, S. N. Valgushev","submitted_at":"2015-05-18T10:24:46Z","abstract_excerpt":"We report on the mean-field study of the Chiral Magnetic Effect (CME) in static magnetic fields within a simple model of a parity-breaking Weyl semimetal given by the lattice Wilson-Dirac Hamiltonian with constant chiral chemical potential. We consider both the mean-field renormalization of the model parameters and nontrivial corrections to the CME originating from re-summed ladder diagrams with arbitrary number of loops. We find that on-site repulsive interactions affect the chiral magnetic conductivity almost exclusively through the enhancement of the renormalized chiral chemical potential. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.04582","kind":"arxiv","version":3},"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":"1505.04582","created_at":"2026-05-18T01:25:18.120123+00:00"},{"alias_kind":"arxiv_version","alias_value":"1505.04582v3","created_at":"2026-05-18T01:25:18.120123+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.04582","created_at":"2026-05-18T01:25:18.120123+00:00"},{"alias_kind":"pith_short_12","alias_value":"D7Z2LJ3UDNLF","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_16","alias_value":"D7Z2LJ3UDNLFWQPD","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_8","alias_value":"D7Z2LJ3U","created_at":"2026-05-18T12:29:17.054201+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/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2","json":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2.json","graph_json":"https://pith.science/api/pith-number/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/graph.json","events_json":"https://pith.science/api/pith-number/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/events.json","paper":"https://pith.science/paper/D7Z2LJ3U"},"agent_actions":{"view_html":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2","download_json":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2.json","view_paper":"https://pith.science/paper/D7Z2LJ3U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1505.04582&json=true","fetch_graph":"https://pith.science/api/pith-number/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/graph.json","fetch_events":"https://pith.science/api/pith-number/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/action/storage_attestation","attest_author":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/action/author_attestation","sign_citation":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/action/citation_signature","submit_replication":"https://pith.science/pith/D7Z2LJ3UDNLFWQPDDXIYRJ5ME2/action/replication_record"}},"created_at":"2026-05-18T01:25:18.120123+00:00","updated_at":"2026-05-18T01:25:18.120123+00:00"}