{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:PLQ7DGWCP44CNTRTRNET2MKF4Q","short_pith_number":"pith:PLQ7DGWC","schema_version":"1.0","canonical_sha256":"7ae1f19ac27f3826ce338b493d3145e43b3a0fd20eb16ca2e500adf4fe4ae50a","source":{"kind":"arxiv","id":"1404.5963","version":1},"attestation_state":"computed","paper":{"title":"Lorentz Invariance in Chiral Kinetic Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dam T. Son, Ho-Ung Yee, Jing-Yuan Chen, Mikhail A. Stephanov, Yi Yin","submitted_at":"2014-04-23T20:00:13Z","abstract_excerpt":"We show that Lorentz invariance is realized nontrivially in the classical action of a massless spin-$\\frac12$ particle with definite helicity. We find that the ordinary Lorentz transformation is modified by a shift orthogonal to the boost vector and the particle momentum. The shift ensures angular momentum conservation in particle collisions and implies a nonlocality of the collision term in the Lorentz-invariant kinetic theory due to side jumps. We show that 2/3 of the chiral-vortical effect for a uniformly rotating particle distribution can be attributed to the magnetic moment coupling requi"},"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":"1404.5963","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-04-23T20:00:13Z","cross_cats_sorted":[],"title_canon_sha256":"08a6b9b254b77cd736ab0e142c2440a8f554a3b671ce4547d1be4f2f5b973e4b","abstract_canon_sha256":"a30b89608a8f08455140309e2224fd8444dba6d32f92074e1c1df6b17dc45e71"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:38:44.207693Z","signature_b64":"1b9Dlrsw++IYWwi9UcRlVo8V0Zt9Ed+XnPv2x9WS3lWAdnrFGz5HXq2FC/FDcIxZ04NZdu8Z6vNMlrjjby5BDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ae1f19ac27f3826ce338b493d3145e43b3a0fd20eb16ca2e500adf4fe4ae50a","last_reissued_at":"2026-05-18T02:38:44.207141Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:38:44.207141Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lorentz Invariance in Chiral Kinetic Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dam T. Son, Ho-Ung Yee, Jing-Yuan Chen, Mikhail A. Stephanov, Yi Yin","submitted_at":"2014-04-23T20:00:13Z","abstract_excerpt":"We show that Lorentz invariance is realized nontrivially in the classical action of a massless spin-$\\frac12$ particle with definite helicity. We find that the ordinary Lorentz transformation is modified by a shift orthogonal to the boost vector and the particle momentum. The shift ensures angular momentum conservation in particle collisions and implies a nonlocality of the collision term in the Lorentz-invariant kinetic theory due to side jumps. We show that 2/3 of the chiral-vortical effect for a uniformly rotating particle distribution can be attributed to the magnetic moment coupling requi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.5963","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":""},"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":"1404.5963","created_at":"2026-05-18T02:38:44.207225+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.5963v1","created_at":"2026-05-18T02:38:44.207225+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.5963","created_at":"2026-05-18T02:38:44.207225+00:00"},{"alias_kind":"pith_short_12","alias_value":"PLQ7DGWCP44C","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"PLQ7DGWCP44CNTRT","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"PLQ7DGWC","created_at":"2026-05-18T12:28:43.426989+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.19817","citing_title":"Spin Hall effect and Berry curvature of gravitons from quantum field theory","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2509.15731","citing_title":"Quantum Metric Corrections to Liouville's Theorem and Chiral Kinetic Theory","ref_index":39,"is_internal_anchor":true},{"citing_arxiv_id":"2604.24410","citing_title":"Chiral Magnetic effect as the anomaly in the transverse axial vector Ward Identity","ref_index":19,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q","json":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q.json","graph_json":"https://pith.science/api/pith-number/PLQ7DGWCP44CNTRTRNET2MKF4Q/graph.json","events_json":"https://pith.science/api/pith-number/PLQ7DGWCP44CNTRTRNET2MKF4Q/events.json","paper":"https://pith.science/paper/PLQ7DGWC"},"agent_actions":{"view_html":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q","download_json":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q.json","view_paper":"https://pith.science/paper/PLQ7DGWC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.5963&json=true","fetch_graph":"https://pith.science/api/pith-number/PLQ7DGWCP44CNTRTRNET2MKF4Q/graph.json","fetch_events":"https://pith.science/api/pith-number/PLQ7DGWCP44CNTRTRNET2MKF4Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q/action/storage_attestation","attest_author":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q/action/author_attestation","sign_citation":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q/action/citation_signature","submit_replication":"https://pith.science/pith/PLQ7DGWCP44CNTRTRNET2MKF4Q/action/replication_record"}},"created_at":"2026-05-18T02:38:44.207225+00:00","updated_at":"2026-05-18T02:38:44.207225+00:00"}