{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:TZPVH7C4DG5LPALHHJ3SRTIW4R","short_pith_number":"pith:TZPVH7C4","schema_version":"1.0","canonical_sha256":"9e5f53fc5c19bab781673a7728cd16e46c354f47392d692249549a9d50e85b6c","source":{"kind":"arxiv","id":"1504.03545","version":2},"attestation_state":"computed","paper":{"title":"A torsional completion of gravity for Dirac matter fields and its applications to neutrino oscillations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Luca Fabbri, Stefano Vignolo","submitted_at":"2015-04-14T13:51:10Z","abstract_excerpt":"In this paper, we consider the torsional completion of gravitation for an underlying background filled with Dirac fields, applying it to the problem of neutrino oscillations: we discuss the effects of the induced torsional interactions as corrections to the neutrino oscillation mechanism."},"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":"1504.03545","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-04-14T13:51:10Z","cross_cats_sorted":[],"title_canon_sha256":"9f43d73ad6777b55fe89db1ac46618ba595abcf1e6240d0f91ab7cf6683c5a99","abstract_canon_sha256":"9fb7399e0be94aa2ae1b74a0f672063011441e81305fa852b64a92c61a10430a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:08.065085Z","signature_b64":"ycqFHn2Klyy+vlP0pJ8WrWgHMMKLvSARdRfzf3ECEkDVQ/afzeM45J/e+Okdie6E+dx/LKd2qu+7FPQlUlc4CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e5f53fc5c19bab781673a7728cd16e46c354f47392d692249549a9d50e85b6c","last_reissued_at":"2026-05-18T01:22:08.064562Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:08.064562Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A torsional completion of gravity for Dirac matter fields and its applications to neutrino oscillations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Luca Fabbri, Stefano Vignolo","submitted_at":"2015-04-14T13:51:10Z","abstract_excerpt":"In this paper, we consider the torsional completion of gravitation for an underlying background filled with Dirac fields, applying it to the problem of neutrino oscillations: we discuss the effects of the induced torsional interactions as corrections to the neutrino oscillation mechanism."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1504.03545","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":"1504.03545","created_at":"2026-05-18T01:22:08.064641+00:00"},{"alias_kind":"arxiv_version","alias_value":"1504.03545v2","created_at":"2026-05-18T01:22:08.064641+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1504.03545","created_at":"2026-05-18T01:22:08.064641+00:00"},{"alias_kind":"pith_short_12","alias_value":"TZPVH7C4DG5L","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_16","alias_value":"TZPVH7C4DG5LPALH","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_8","alias_value":"TZPVH7C4","created_at":"2026-05-18T12:29:44.643036+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/TZPVH7C4DG5LPALHHJ3SRTIW4R","json":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R.json","graph_json":"https://pith.science/api/pith-number/TZPVH7C4DG5LPALHHJ3SRTIW4R/graph.json","events_json":"https://pith.science/api/pith-number/TZPVH7C4DG5LPALHHJ3SRTIW4R/events.json","paper":"https://pith.science/paper/TZPVH7C4"},"agent_actions":{"view_html":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R","download_json":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R.json","view_paper":"https://pith.science/paper/TZPVH7C4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1504.03545&json=true","fetch_graph":"https://pith.science/api/pith-number/TZPVH7C4DG5LPALHHJ3SRTIW4R/graph.json","fetch_events":"https://pith.science/api/pith-number/TZPVH7C4DG5LPALHHJ3SRTIW4R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R/action/storage_attestation","attest_author":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R/action/author_attestation","sign_citation":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R/action/citation_signature","submit_replication":"https://pith.science/pith/TZPVH7C4DG5LPALHHJ3SRTIW4R/action/replication_record"}},"created_at":"2026-05-18T01:22:08.064641+00:00","updated_at":"2026-05-18T01:22:08.064641+00:00"}