{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:KA75YHBEAZ7CXR5OKPQLBI537Z","short_pith_number":"pith:KA75YHBE","schema_version":"1.0","canonical_sha256":"503fdc1c24067e2bc7ae53e0b0a3bbfe5c87c9e89402921d222411c9116ab664","source":{"kind":"arxiv","id":"hep-ph/0607284","version":1},"attestation_state":"computed","paper":{"title":"Determining Neutrino Mass Hierarchy by Precision Measurements in Electron and Muon Neutrino Disappearance Experiments","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H. Minakata, H. Nunokawa, R. Zukanovich Funchal, S.J. Parke","submitted_at":"2006-07-25T23:27:00Z","abstract_excerpt":"Recently a new method for determining the neutrino mass hierarchy by comparing the effective values of the atmospheric \\Delta m^2 measured in the electron neutrino disappearance channel, \\Delta m^2(ee), with the one measured in the muon neutrino disappearance channel, \\Delta m^2(\\mu \\mu), was proposed. If \\Delta m^2(ee) is larger (smaller) than \\Delta m^2(\\mu \\mu) the hierarchy is of the normal (inverted) type. We re-examine this proposition in the light of two very high precision measurements: \\Delta m^2(\\mu \\mu) that may be accomplished by the phase II of the Tokai-to-Kamioka (T2K) experimen"},"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":"hep-ph/0607284","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-07-25T23:27:00Z","cross_cats_sorted":[],"title_canon_sha256":"2fb7b837880d637766e2ce6feafee242eb895bc0a2f99fa530245af256487011","abstract_canon_sha256":"626bcc54594dc3faf2f1b8f135cc9e09feca5c38d5e41a36ed34db52fec00c0b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:28:50.553431Z","signature_b64":"JpaXb0icDLv27OMptWBzNSlKWuGPpEoNbiuIUGD0M64HNIEEisP2aB363AqalKVLCkOmGuuy7I0WfyqBJRYjBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"503fdc1c24067e2bc7ae53e0b0a3bbfe5c87c9e89402921d222411c9116ab664","last_reissued_at":"2026-07-04T15:28:50.552822Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:28:50.552822Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Determining Neutrino Mass Hierarchy by Precision Measurements in Electron and Muon Neutrino Disappearance Experiments","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H. Minakata, H. Nunokawa, R. Zukanovich Funchal, S.J. Parke","submitted_at":"2006-07-25T23:27:00Z","abstract_excerpt":"Recently a new method for determining the neutrino mass hierarchy by comparing the effective values of the atmospheric \\Delta m^2 measured in the electron neutrino disappearance channel, \\Delta m^2(ee), with the one measured in the muon neutrino disappearance channel, \\Delta m^2(\\mu \\mu), was proposed. If \\Delta m^2(ee) is larger (smaller) than \\Delta m^2(\\mu \\mu) the hierarchy is of the normal (inverted) type. We re-examine this proposition in the light of two very high precision measurements: \\Delta m^2(\\mu \\mu) that may be accomplished by the phase II of the Tokai-to-Kamioka (T2K) experimen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0607284","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0607284/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-ph/0607284","created_at":"2026-07-04T15:28:50.552882+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0607284v1","created_at":"2026-07-04T15:28:50.552882+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0607284","created_at":"2026-07-04T15:28:50.552882+00:00"},{"alias_kind":"pith_short_12","alias_value":"KA75YHBEAZ7C","created_at":"2026-07-04T15:28:50.552882+00:00"},{"alias_kind":"pith_short_16","alias_value":"KA75YHBEAZ7CXR5O","created_at":"2026-07-04T15:28:50.552882+00:00"},{"alias_kind":"pith_short_8","alias_value":"KA75YHBE","created_at":"2026-07-04T15:28:50.552882+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.24560","citing_title":"Disentangle RG Running Parameters with Medium-Baseline Reactor Experiments","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2601.09791","citing_title":"Lessons from the first JUNO results","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2410.05380","citing_title":"NuFit-6.0: Updated global analysis of three-flavor neutrino oscillations","ref_index":20,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z","json":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z.json","graph_json":"https://pith.science/api/pith-number/KA75YHBEAZ7CXR5OKPQLBI537Z/graph.json","events_json":"https://pith.science/api/pith-number/KA75YHBEAZ7CXR5OKPQLBI537Z/events.json","paper":"https://pith.science/paper/KA75YHBE"},"agent_actions":{"view_html":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z","download_json":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z.json","view_paper":"https://pith.science/paper/KA75YHBE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0607284&json=true","fetch_graph":"https://pith.science/api/pith-number/KA75YHBEAZ7CXR5OKPQLBI537Z/graph.json","fetch_events":"https://pith.science/api/pith-number/KA75YHBEAZ7CXR5OKPQLBI537Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z/action/storage_attestation","attest_author":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z/action/author_attestation","sign_citation":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z/action/citation_signature","submit_replication":"https://pith.science/pith/KA75YHBEAZ7CXR5OKPQLBI537Z/action/replication_record"}},"created_at":"2026-07-04T15:28:50.552882+00:00","updated_at":"2026-07-04T15:28:50.552882+00:00"}