{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:W5B6ITYC26O5UFFLEPGVGUCN5I","short_pith_number":"pith:W5B6ITYC","schema_version":"1.0","canonical_sha256":"b743e44f02d79dda14ab23cd53504dea3018faeaf7b2e269055b972900c86bc1","source":{"kind":"arxiv","id":"1405.0416","version":3},"attestation_state":"computed","paper":{"title":"The Daya Bay and T2K results on $\\sin^2 2 \\theta_{13}$ and Non-Standard Neutrino Interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. Meloni, I. Girardi, S. T. Petcov","submitted_at":"2014-05-02T14:35:24Z","abstract_excerpt":"We show that the relatively large best fit value of $\\sin^2 2 \\theta_{13} = 0.14 \\, (0.17)$ measured in the T2K experiment for fixed values of i) the Dirac CP violation phase $\\delta = 0$, and ii) the atmospheric neutrino mixing parameters $\\theta_{23} = \\pi/4$, $|\\Delta m^2_{32}| = 2.4 \\times 10^{-3} \\; {\\rm eV}^2$, can be reconciled with the Daya Bay result $\\sin^2 2 \\theta_{13} = 0.090 \\pm 0.009$ if the effects of non-standard neutrino interactions (NSI) in the relevant $\\bar \\nu_e \\to \\bar \\nu_e$ and $\\nu_\\mu \\to \\nu_e$ oscillation probabilities are taken into account."},"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":"1405.0416","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-02T14:35:24Z","cross_cats_sorted":[],"title_canon_sha256":"9999f62b8efa7df7bec10ec7f1c1ba10a6bb9c2fceaa832ccdc04c65bedd2250","abstract_canon_sha256":"320bf4b60b1ae43d73c8559d4320855dbf0d1e4efa6c767999cae7ea30554403"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:45:31.377176Z","signature_b64":"cMe4qn6fsLCwnOpAFh2LpxeqYHl/XkixGbRBYSepvjKAMrMGaf/B/sVednuh0ENRBhH18Ax5YRWm/ozk4yAzBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b743e44f02d79dda14ab23cd53504dea3018faeaf7b2e269055b972900c86bc1","last_reissued_at":"2026-05-18T02:45:31.376612Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:45:31.376612Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Daya Bay and T2K results on $\\sin^2 2 \\theta_{13}$ and Non-Standard Neutrino Interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. Meloni, I. Girardi, S. T. Petcov","submitted_at":"2014-05-02T14:35:24Z","abstract_excerpt":"We show that the relatively large best fit value of $\\sin^2 2 \\theta_{13} = 0.14 \\, (0.17)$ measured in the T2K experiment for fixed values of i) the Dirac CP violation phase $\\delta = 0$, and ii) the atmospheric neutrino mixing parameters $\\theta_{23} = \\pi/4$, $|\\Delta m^2_{32}| = 2.4 \\times 10^{-3} \\; {\\rm eV}^2$, can be reconciled with the Daya Bay result $\\sin^2 2 \\theta_{13} = 0.090 \\pm 0.009$ if the effects of non-standard neutrino interactions (NSI) in the relevant $\\bar \\nu_e \\to \\bar \\nu_e$ and $\\nu_\\mu \\to \\nu_e$ oscillation probabilities are taken into account."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.0416","kind":"arxiv","version":3},"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":"1405.0416","created_at":"2026-05-18T02:45:31.376683+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.0416v3","created_at":"2026-05-18T02:45:31.376683+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.0416","created_at":"2026-05-18T02:45:31.376683+00:00"},{"alias_kind":"pith_short_12","alias_value":"W5B6ITYC26O5","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"W5B6ITYC26O5UFFL","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"W5B6ITYC","created_at":"2026-05-18T12:28:54.890064+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/W5B6ITYC26O5UFFLEPGVGUCN5I","json":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I.json","graph_json":"https://pith.science/api/pith-number/W5B6ITYC26O5UFFLEPGVGUCN5I/graph.json","events_json":"https://pith.science/api/pith-number/W5B6ITYC26O5UFFLEPGVGUCN5I/events.json","paper":"https://pith.science/paper/W5B6ITYC"},"agent_actions":{"view_html":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I","download_json":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I.json","view_paper":"https://pith.science/paper/W5B6ITYC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.0416&json=true","fetch_graph":"https://pith.science/api/pith-number/W5B6ITYC26O5UFFLEPGVGUCN5I/graph.json","fetch_events":"https://pith.science/api/pith-number/W5B6ITYC26O5UFFLEPGVGUCN5I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I/action/storage_attestation","attest_author":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I/action/author_attestation","sign_citation":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I/action/citation_signature","submit_replication":"https://pith.science/pith/W5B6ITYC26O5UFFLEPGVGUCN5I/action/replication_record"}},"created_at":"2026-05-18T02:45:31.376683+00:00","updated_at":"2026-05-18T02:45:31.376683+00:00"}