{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:MVF2GW3WQAY3PTR6IYNQFS5YGU","short_pith_number":"pith:MVF2GW3W","schema_version":"1.0","canonical_sha256":"654ba35b768031b7ce3e461b02cbb83504c29b03a243f3d1d983dd95e68e6cfe","source":{"kind":"arxiv","id":"1309.2628","version":2},"attestation_state":"computed","paper":{"title":"Neutrino Quantum Kinetics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"hep-ph","authors_text":"Alexey Vlasenko, George M. Fuller, Vincenzo Cirigliano","submitted_at":"2013-09-10T19:52:12Z","abstract_excerpt":"We present a formulation of the quantum kinetic equations (QKEs) which govern the evolution of neutrino flavor at high density and temperature. Here, the QKEs are derived from the ground up, using fundamental neutrino interactions and quantum field theory. We show that the resulting QKEs describe coherent flavor evolution with an effective mass when inelastic scattering is negligible. The QKEs also contain a collision term. This term can reduce to the collision term in the Boltzmann equation when scattering is dominant and the neutrino effective masses and density matrices become diagonal in t"},"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":"1309.2628","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-09-10T19:52:12Z","cross_cats_sorted":["astro-ph.SR"],"title_canon_sha256":"54e11fe697244a139787314c2636694d35851af40103c0315e3eb6aeac9897bb","abstract_canon_sha256":"92b86c4c85a5b2050b639b770a2f441237861a2d5ca9fb331d0fe5a290fe82c2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:49:12.206632Z","signature_b64":"fVu04kN1PQd/9eEIr9theDSV9vc7lBHPH8D1UVGbjt28dDk+59tjyguVQUigF0qgBiv3+3HZWeO5p486mpjODA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"654ba35b768031b7ce3e461b02cbb83504c29b03a243f3d1d983dd95e68e6cfe","last_reissued_at":"2026-05-18T02:49:12.206035Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:49:12.206035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Neutrino Quantum Kinetics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR"],"primary_cat":"hep-ph","authors_text":"Alexey Vlasenko, George M. Fuller, Vincenzo Cirigliano","submitted_at":"2013-09-10T19:52:12Z","abstract_excerpt":"We present a formulation of the quantum kinetic equations (QKEs) which govern the evolution of neutrino flavor at high density and temperature. Here, the QKEs are derived from the ground up, using fundamental neutrino interactions and quantum field theory. We show that the resulting QKEs describe coherent flavor evolution with an effective mass when inelastic scattering is negligible. The QKEs also contain a collision term. This term can reduce to the collision term in the Boltzmann equation when scattering is dominant and the neutrino effective masses and density matrices become diagonal in t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1309.2628","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":"1309.2628","created_at":"2026-05-18T02:49:12.206125+00:00"},{"alias_kind":"arxiv_version","alias_value":"1309.2628v2","created_at":"2026-05-18T02:49:12.206125+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1309.2628","created_at":"2026-05-18T02:49:12.206125+00:00"},{"alias_kind":"pith_short_12","alias_value":"MVF2GW3WQAY3","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_16","alias_value":"MVF2GW3WQAY3PTR6","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_8","alias_value":"MVF2GW3W","created_at":"2026-05-18T12:27:52.871228+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.25687","citing_title":"Collective neutrino-antineutrino pair oscillations","ref_index":114,"is_internal_anchor":false},{"citing_arxiv_id":"2604.06404","citing_title":"Neutrino transport and flavor instabilities in a post-merger disk","ref_index":105,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU","json":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU.json","graph_json":"https://pith.science/api/pith-number/MVF2GW3WQAY3PTR6IYNQFS5YGU/graph.json","events_json":"https://pith.science/api/pith-number/MVF2GW3WQAY3PTR6IYNQFS5YGU/events.json","paper":"https://pith.science/paper/MVF2GW3W"},"agent_actions":{"view_html":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU","download_json":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU.json","view_paper":"https://pith.science/paper/MVF2GW3W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1309.2628&json=true","fetch_graph":"https://pith.science/api/pith-number/MVF2GW3WQAY3PTR6IYNQFS5YGU/graph.json","fetch_events":"https://pith.science/api/pith-number/MVF2GW3WQAY3PTR6IYNQFS5YGU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU/action/storage_attestation","attest_author":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU/action/author_attestation","sign_citation":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU/action/citation_signature","submit_replication":"https://pith.science/pith/MVF2GW3WQAY3PTR6IYNQFS5YGU/action/replication_record"}},"created_at":"2026-05-18T02:49:12.206125+00:00","updated_at":"2026-05-18T02:49:12.206125+00:00"}