{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:QQ5VSOU7OUQAZHP4I7HHA7CWOR","short_pith_number":"pith:QQ5VSOU7","schema_version":"1.0","canonical_sha256":"843b593a9f75200c9dfc47ce707c567479247da926037772338522019a2ef1e1","source":{"kind":"arxiv","id":"2202.13358","version":3},"attestation_state":"computed","paper":{"title":"Heavy Majorana neutrino pair production from $Z^\\prime$ at hadron and lepton colliders","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arindam Das, Sanjoy Mandal, Sujay Shil, Takaaki Nomura","submitted_at":"2022-02-27T13:18:08Z","abstract_excerpt":"A gauged U$(1)$ extension of the Standard Model (SM) is a simple and anomaly free framework where three generations of Majorana type right-handed neutrinos (RHNs) are introduced to generate light neutrino mass and flavor mixings through the seesaw mechanism. We investigate such models at different hadron and lepton colliders via $Z^\\prime$ induced Majorana type RHNs pair production. We derive bounds on U$(1)$ gauge coupling $(g^\\prime)$ comparing the model cross sections with experimentally observed data for different $Z^\\prime$ mass $(M_{Z^\\prime})$ and RHNs mass $(M_N)$. Using these limits w"},"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":"2202.13358","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-27T13:18:08Z","cross_cats_sorted":[],"title_canon_sha256":"527bb4d1acb595a44b9dfa61fbc5337a54ec07fba403e102b264c0b63c412640","abstract_canon_sha256":"15cd3b662f80c33d830b57b6ebfdea362329b05910e35e10db2567e334e5c10d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:30:55.286489Z","signature_b64":"pjwZCA9TrxkpiDK4f1IysU48Qx2EEdkcXkA9y0BLfvr2naa5XbJWXMbfq2u6VFGkn0LqViiRpZv+Rswi08mRAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"843b593a9f75200c9dfc47ce707c567479247da926037772338522019a2ef1e1","last_reissued_at":"2026-07-05T04:30:55.286046Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:30:55.286046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heavy Majorana neutrino pair production from $Z^\\prime$ at hadron and lepton colliders","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Arindam Das, Sanjoy Mandal, Sujay Shil, Takaaki Nomura","submitted_at":"2022-02-27T13:18:08Z","abstract_excerpt":"A gauged U$(1)$ extension of the Standard Model (SM) is a simple and anomaly free framework where three generations of Majorana type right-handed neutrinos (RHNs) are introduced to generate light neutrino mass and flavor mixings through the seesaw mechanism. We investigate such models at different hadron and lepton colliders via $Z^\\prime$ induced Majorana type RHNs pair production. We derive bounds on U$(1)$ gauge coupling $(g^\\prime)$ comparing the model cross sections with experimentally observed data for different $Z^\\prime$ mass $(M_{Z^\\prime})$ and RHNs mass $(M_N)$. Using these limits w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.13358","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2202.13358/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":"2202.13358","created_at":"2026-07-05T04:30:55.286103+00:00"},{"alias_kind":"arxiv_version","alias_value":"2202.13358v3","created_at":"2026-07-05T04:30:55.286103+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.13358","created_at":"2026-07-05T04:30:55.286103+00:00"},{"alias_kind":"pith_short_12","alias_value":"QQ5VSOU7OUQA","created_at":"2026-07-05T04:30:55.286103+00:00"},{"alias_kind":"pith_short_16","alias_value":"QQ5VSOU7OUQAZHP4","created_at":"2026-07-05T04:30:55.286103+00:00"},{"alias_kind":"pith_short_8","alias_value":"QQ5VSOU7","created_at":"2026-07-05T04:30:55.286103+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.19751","citing_title":"Right-handed neutrino production through first-generation leptoquarks","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR","json":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR.json","graph_json":"https://pith.science/api/pith-number/QQ5VSOU7OUQAZHP4I7HHA7CWOR/graph.json","events_json":"https://pith.science/api/pith-number/QQ5VSOU7OUQAZHP4I7HHA7CWOR/events.json","paper":"https://pith.science/paper/QQ5VSOU7"},"agent_actions":{"view_html":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR","download_json":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR.json","view_paper":"https://pith.science/paper/QQ5VSOU7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2202.13358&json=true","fetch_graph":"https://pith.science/api/pith-number/QQ5VSOU7OUQAZHP4I7HHA7CWOR/graph.json","fetch_events":"https://pith.science/api/pith-number/QQ5VSOU7OUQAZHP4I7HHA7CWOR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR/action/storage_attestation","attest_author":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR/action/author_attestation","sign_citation":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR/action/citation_signature","submit_replication":"https://pith.science/pith/QQ5VSOU7OUQAZHP4I7HHA7CWOR/action/replication_record"}},"created_at":"2026-07-05T04:30:55.286103+00:00","updated_at":"2026-07-05T04:30:55.286103+00:00"}