{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:42QA2GAELY4JC6H4SS63H7P44C","short_pith_number":"pith:42QA2GAE","schema_version":"1.0","canonical_sha256":"e6a00d18045e389178fc94bdb3fdfce0b4ab0fa40a7bcc0a808dc30b4fad8b60","source":{"kind":"arxiv","id":"1105.3188","version":2},"attestation_state":"computed","paper":{"title":"TeV Scale Models of Neutrino Masses and Their Phenomenology","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Jinrui Huang, Mu-Chun Chen","submitted_at":"2011-05-16T20:00:00Z","abstract_excerpt":"We review various TeV scale models for neutrino masses utilizing different types of seesaw mechanisms, higher dimensional operators, expanded gauge symmetries, or low scale extra dimensions. In addition, we discuss the implications of these models for the collider experiments and low energy lepton flavor violation searches."},"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":"1105.3188","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-05-16T20:00:00Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"92c2106e7823902bb888f12f109a4831b954edb94520e32df23d37e086cd7bb2","abstract_canon_sha256":"1ddb140259396219a631db5a68c6081647854c0b42f8bf771ba63e2ffe319d36"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:21:59.985690Z","signature_b64":"Z4VQQO6mx/8wvkmvQRiBLvgrpnGlGQHpJhQNWrBDteAuTDt1FfpeqZHrOiXAMhyD0YcJpDuFKsuLyuyClplHDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e6a00d18045e389178fc94bdb3fdfce0b4ab0fa40a7bcc0a808dc30b4fad8b60","last_reissued_at":"2026-05-18T02:21:59.985082Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:21:59.985082Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"TeV Scale Models of Neutrino Masses and Their Phenomenology","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Jinrui Huang, Mu-Chun Chen","submitted_at":"2011-05-16T20:00:00Z","abstract_excerpt":"We review various TeV scale models for neutrino masses utilizing different types of seesaw mechanisms, higher dimensional operators, expanded gauge symmetries, or low scale extra dimensions. In addition, we discuss the implications of these models for the collider experiments and low energy lepton flavor violation searches."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.3188","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":"1105.3188","created_at":"2026-05-18T02:21:59.985178+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.3188v2","created_at":"2026-05-18T02:21:59.985178+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.3188","created_at":"2026-05-18T02:21:59.985178+00:00"},{"alias_kind":"pith_short_12","alias_value":"42QA2GAELY4J","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"42QA2GAELY4JC6H4","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"42QA2GAE","created_at":"2026-05-18T12:26:20.644004+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/42QA2GAELY4JC6H4SS63H7P44C","json":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C.json","graph_json":"https://pith.science/api/pith-number/42QA2GAELY4JC6H4SS63H7P44C/graph.json","events_json":"https://pith.science/api/pith-number/42QA2GAELY4JC6H4SS63H7P44C/events.json","paper":"https://pith.science/paper/42QA2GAE"},"agent_actions":{"view_html":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C","download_json":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C.json","view_paper":"https://pith.science/paper/42QA2GAE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.3188&json=true","fetch_graph":"https://pith.science/api/pith-number/42QA2GAELY4JC6H4SS63H7P44C/graph.json","fetch_events":"https://pith.science/api/pith-number/42QA2GAELY4JC6H4SS63H7P44C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C/action/storage_attestation","attest_author":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C/action/author_attestation","sign_citation":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C/action/citation_signature","submit_replication":"https://pith.science/pith/42QA2GAELY4JC6H4SS63H7P44C/action/replication_record"}},"created_at":"2026-05-18T02:21:59.985178+00:00","updated_at":"2026-05-18T02:21:59.985178+00:00"}