{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:VGFPEPCGX6VR5ZPP4IYLNXC2ZQ","short_pith_number":"pith:VGFPEPCG","schema_version":"1.0","canonical_sha256":"a98af23c46bfab1ee5efe230b6dc5acc35779666e0eca5a5ac1e51e90904bc06","source":{"kind":"arxiv","id":"2608.08269","version":1},"attestation_state":"computed","paper":{"title":"Quantum Formulation of Chiral Vortical Effect in Weyl Semi-metals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"B. Q. Song","submitted_at":"2026-08-08T17:59:12Z","abstract_excerpt":"The chiral vortical effect (CVE) is the generation of an axial current in a rotating Weyl fermion; its description is presently based on semiclassical frameworks. In this work, we develop a fully quantum formulation for CVE, solving the exact evolution of microscopic spinful wavefunctions, which enables a bottom-up quantitative test of semi-classical theories and postulated distributions $f_{\\text{CVE}}$ in different reference frames. Notably, it shows that $f_{\\text{CVE}}$ is over a ground-state-free Floquet spectrum, qualitatively distinct from a thermal equilibrium distribution (i.e., fermi"},"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":"2608.08269","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-08-08T17:59:12Z","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"title_canon_sha256":"e3179b1964b2af4338617435c2cfc42f03e49e26c1eb51fc69cf68bdb90c4cb2","abstract_canon_sha256":"75cca211986a38981607ffffb7ee36d80f44c6ef1181e25df4981c9a1f2caff5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-11T01:22:10.409961Z","signature_b64":"VVLqt/Z96syMhidasBWrSRvBvO6f7DYYgGZ9cZ3gRZSFf75XR1TMvmnCTIynuUWwzxHBUa99idh9CfVYRkS1CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a98af23c46bfab1ee5efe230b6dc5acc35779666e0eca5a5ac1e51e90904bc06","last_reissued_at":"2026-08-11T01:22:10.407592Z","signature_status":"signed_v1","first_computed_at":"2026-08-11T01:22:10.407592Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Formulation of Chiral Vortical Effect in Weyl Semi-metals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"B. Q. Song","submitted_at":"2026-08-08T17:59:12Z","abstract_excerpt":"The chiral vortical effect (CVE) is the generation of an axial current in a rotating Weyl fermion; its description is presently based on semiclassical frameworks. In this work, we develop a fully quantum formulation for CVE, solving the exact evolution of microscopic spinful wavefunctions, which enables a bottom-up quantitative test of semi-classical theories and postulated distributions $f_{\\text{CVE}}$ in different reference frames. Notably, it shows that $f_{\\text{CVE}}$ is over a ground-state-free Floquet spectrum, qualitatively distinct from a thermal equilibrium distribution (i.e., fermi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.08269","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/2608.08269/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":"2608.08269","created_at":"2026-08-11T01:22:10.408297+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.08269v1","created_at":"2026-08-11T01:22:10.408297+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.08269","created_at":"2026-08-11T01:22:10.408297+00:00"},{"alias_kind":"pith_short_12","alias_value":"VGFPEPCGX6VR","created_at":"2026-08-11T01:22:10.408297+00:00"},{"alias_kind":"pith_short_16","alias_value":"VGFPEPCGX6VR5ZPP","created_at":"2026-08-11T01:22:10.408297+00:00"},{"alias_kind":"pith_short_8","alias_value":"VGFPEPCG","created_at":"2026-08-11T01:22:10.408297+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/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ","json":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ.json","graph_json":"https://pith.science/api/pith-number/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/graph.json","events_json":"https://pith.science/api/pith-number/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/events.json","paper":"https://pith.science/paper/VGFPEPCG"},"agent_actions":{"view_html":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ","download_json":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ.json","view_paper":"https://pith.science/paper/VGFPEPCG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.08269&json=true","fetch_graph":"https://pith.science/api/pith-number/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/graph.json","fetch_events":"https://pith.science/api/pith-number/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/action/storage_attestation","attest_author":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/action/author_attestation","sign_citation":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/action/citation_signature","submit_replication":"https://pith.science/pith/VGFPEPCGX6VR5ZPP4IYLNXC2ZQ/action/replication_record"}},"created_at":"2026-08-11T01:22:10.408297+00:00","updated_at":"2026-08-11T01:22:10.408297+00:00"}