{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:4JVIXCWZX5ILTDUJ2CCKUKW5AS","short_pith_number":"pith:4JVIXCWZ","schema_version":"1.0","canonical_sha256":"e26a8b8ad9bf50b98e89d084aa2add048353d6f37be1143e77ad13213acc8656","source":{"kind":"arxiv","id":"1507.04366","version":1},"attestation_state":"computed","paper":{"title":"Bayesian global analysis of neutrino oscillation data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Johannes Bergstrom, M. C. Gonzalez-Garcia, Michele Maltoni, Thomas Schwetz","submitted_at":"2015-07-15T20:04:26Z","abstract_excerpt":"We perform a Bayesian analysis of current neutrino oscillation data. When estimating the oscillation parameters we find that the results generally agree with those of the $\\chi^2$ method, with some differences involving $s_{23}^2$ and CP-violating effects. We discuss the additional subtleties caused by the circular nature of the CP-violating phase, and how it is possible to obtain correlation coefficients with $s_{23}^2$. When performing model comparison, we find that there is no significant evidence for any mass ordering, any octant of $s_{23}^2$ or a deviation from maximal mixing, nor the pr"},"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":"1507.04366","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-07-15T20:04:26Z","cross_cats_sorted":[],"title_canon_sha256":"6174a3bc7d810959eca8bbf3d08cad0dfcb5b0705089cd9e8d16a0c91f27f8a6","abstract_canon_sha256":"41b4c0917be313c7b4d36c65e1ad26ce161cbcd6a5c4ab7530cf88b8235257c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:29:38.088710Z","signature_b64":"7DDoihV51Zhe5ImhkRyi4HD3fpZ8aOME376ahqe1JxviTWx8bF6A374ZX55ZzNxS3T/o8ciJtb0rg59mMNLfAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e26a8b8ad9bf50b98e89d084aa2add048353d6f37be1143e77ad13213acc8656","last_reissued_at":"2026-05-18T01:29:38.088103Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:29:38.088103Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bayesian global analysis of neutrino oscillation data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Johannes Bergstrom, M. C. Gonzalez-Garcia, Michele Maltoni, Thomas Schwetz","submitted_at":"2015-07-15T20:04:26Z","abstract_excerpt":"We perform a Bayesian analysis of current neutrino oscillation data. When estimating the oscillation parameters we find that the results generally agree with those of the $\\chi^2$ method, with some differences involving $s_{23}^2$ and CP-violating effects. We discuss the additional subtleties caused by the circular nature of the CP-violating phase, and how it is possible to obtain correlation coefficients with $s_{23}^2$. When performing model comparison, we find that there is no significant evidence for any mass ordering, any octant of $s_{23}^2$ or a deviation from maximal mixing, nor the pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.04366","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":"1507.04366","created_at":"2026-05-18T01:29:38.088196+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.04366v1","created_at":"2026-05-18T01:29:38.088196+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.04366","created_at":"2026-05-18T01:29:38.088196+00:00"},{"alias_kind":"pith_short_12","alias_value":"4JVIXCWZX5IL","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_16","alias_value":"4JVIXCWZX5ILTDUJ","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_8","alias_value":"4JVIXCWZ","created_at":"2026-05-18T12:29:05.191682+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.25557","citing_title":"Jarvis-HEP: A lightweight Python framework for workflow composition and parameter scans in high-energy physics","ref_index":117,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS","json":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS.json","graph_json":"https://pith.science/api/pith-number/4JVIXCWZX5ILTDUJ2CCKUKW5AS/graph.json","events_json":"https://pith.science/api/pith-number/4JVIXCWZX5ILTDUJ2CCKUKW5AS/events.json","paper":"https://pith.science/paper/4JVIXCWZ"},"agent_actions":{"view_html":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS","download_json":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS.json","view_paper":"https://pith.science/paper/4JVIXCWZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.04366&json=true","fetch_graph":"https://pith.science/api/pith-number/4JVIXCWZX5ILTDUJ2CCKUKW5AS/graph.json","fetch_events":"https://pith.science/api/pith-number/4JVIXCWZX5ILTDUJ2CCKUKW5AS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS/action/storage_attestation","attest_author":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS/action/author_attestation","sign_citation":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS/action/citation_signature","submit_replication":"https://pith.science/pith/4JVIXCWZX5ILTDUJ2CCKUKW5AS/action/replication_record"}},"created_at":"2026-05-18T01:29:38.088196+00:00","updated_at":"2026-05-18T01:29:38.088196+00:00"}