{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:Q7KFSYDRBARLAR7TAVZL6HAX3M","short_pith_number":"pith:Q7KFSYDR","schema_version":"1.0","canonical_sha256":"87d45960710822b047f30572bf1c17db0dbbba98600bc36af9b3ec3a46c9f2ec","source":{"kind":"arxiv","id":"1802.09251","version":1},"attestation_state":"computed","paper":{"title":"Phenomenology of the Higgs sector of a Dimension-7 Neutrino Mass Generation Mechanism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"S. Nandi, Sudip Jana, Tathagata Ghosh","submitted_at":"2018-02-26T11:30:23Z","abstract_excerpt":"In this paper, we revisit the dimension-7 neutrino mass generation mechanism based on the addition of an isospin $3/2$ scalar quadruplet and two vector-like iso-triplet leptons to the standard model. We discuss the LHC phenomenology of the charged scalars of this model, complemented by the electroweak precision and lepton flavor violation constraints. We pay particular attention to the triply charged and doubly charged components. We focus on the same-sign-tri-lepton signatures originating from the triply-charged scalars and find a discovery reach of 600 - 950 GeV at 3 ab$^{-1}$ of integrated "},"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":"1802.09251","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-02-26T11:30:23Z","cross_cats_sorted":[],"title_canon_sha256":"4a73078b6be384dfa9a0b98cd7b74b9539d557a69e406f4dd92a82168cf65baf","abstract_canon_sha256":"52c697a5b4f3bdf2b78b09432934396b571e419564bddfbe4e6a64ae674e2edb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:12:18.173206Z","signature_b64":"6u1j6p0FCZ6ZdZPW6hreYdcytOIOKqOoJV74ZjLxsgwQQf3JnrWsAnlOnTNHxlESApEe9Il7xQvwDm6t1sP+BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"87d45960710822b047f30572bf1c17db0dbbba98600bc36af9b3ec3a46c9f2ec","last_reissued_at":"2026-05-18T00:12:18.172535Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:12:18.172535Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phenomenology of the Higgs sector of a Dimension-7 Neutrino Mass Generation Mechanism","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"S. Nandi, Sudip Jana, Tathagata Ghosh","submitted_at":"2018-02-26T11:30:23Z","abstract_excerpt":"In this paper, we revisit the dimension-7 neutrino mass generation mechanism based on the addition of an isospin $3/2$ scalar quadruplet and two vector-like iso-triplet leptons to the standard model. We discuss the LHC phenomenology of the charged scalars of this model, complemented by the electroweak precision and lepton flavor violation constraints. We pay particular attention to the triply charged and doubly charged components. We focus on the same-sign-tri-lepton signatures originating from the triply-charged scalars and find a discovery reach of 600 - 950 GeV at 3 ab$^{-1}$ of integrated "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.09251","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":"1802.09251","created_at":"2026-05-18T00:12:18.172642+00:00"},{"alias_kind":"arxiv_version","alias_value":"1802.09251v1","created_at":"2026-05-18T00:12:18.172642+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.09251","created_at":"2026-05-18T00:12:18.172642+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q7KFSYDRBARL","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q7KFSYDRBARLAR7T","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q7KFSYDR","created_at":"2026-05-18T12:32:46.962924+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.02128","citing_title":"Vacuum structure of the Babu-Nandi-Tavartkiladze model of neutrino mass generation","ref_index":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M","json":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M.json","graph_json":"https://pith.science/api/pith-number/Q7KFSYDRBARLAR7TAVZL6HAX3M/graph.json","events_json":"https://pith.science/api/pith-number/Q7KFSYDRBARLAR7TAVZL6HAX3M/events.json","paper":"https://pith.science/paper/Q7KFSYDR"},"agent_actions":{"view_html":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M","download_json":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M.json","view_paper":"https://pith.science/paper/Q7KFSYDR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1802.09251&json=true","fetch_graph":"https://pith.science/api/pith-number/Q7KFSYDRBARLAR7TAVZL6HAX3M/graph.json","fetch_events":"https://pith.science/api/pith-number/Q7KFSYDRBARLAR7TAVZL6HAX3M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M/action/storage_attestation","attest_author":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M/action/author_attestation","sign_citation":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M/action/citation_signature","submit_replication":"https://pith.science/pith/Q7KFSYDRBARLAR7TAVZL6HAX3M/action/replication_record"}},"created_at":"2026-05-18T00:12:18.172642+00:00","updated_at":"2026-05-18T00:12:18.172642+00:00"}