{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:IBUC5SA7CNGLM7KLDUUQPR2QUN","short_pith_number":"pith:IBUC5SA7","schema_version":"1.0","canonical_sha256":"40682ec81f134cb67d4b1d2907c750a3625fab38135518d69a9baf10488d4526","source":{"kind":"arxiv","id":"1607.01910","version":2},"attestation_state":"computed","paper":{"title":"Neutrino Mass Generation and 750 GeV Diphoton excess via photon-photon fusion at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kirtiman Ghosh, S. Nandi, Sudip Jana","submitted_at":"2016-07-07T08:26:11Z","abstract_excerpt":"We propose a new model for explaining the diphoton excess observed at the LHC. The uniqueness of our model is that this excess is being produced by photon-photon induced sub-process. The model includes an isospin $3/2$ scalar multiplet (having triply, doubly and singly charged scalars) at the electroweak (EW) scale to explain the observed neutrino masses via the effective dimension $7$ operator. The model also include a singlet scalar which is the di-photon resonance. The loop induced coupling of the singlet scalar with a pair of photons is enhanced due to contributions from multi-charged EW-s"},"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":"1607.01910","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-07-07T08:26:11Z","cross_cats_sorted":[],"title_canon_sha256":"f91105151777d7b75e0975b6769bbb1ceecc2267271da41d5482221dd48103b8","abstract_canon_sha256":"e8d7b601d8ca5df9a533d745a67afc774c425b6018a1564c27670b9f428aba79"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:21.174065Z","signature_b64":"YNPXYgaknHRuP4X3bc5CLWUcM5Da6OP3N0B+eA5W0EFC81SmDi1ZJReDcJPFUIwdOG9QusIpYIAfcLpGsskRCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"40682ec81f134cb67d4b1d2907c750a3625fab38135518d69a9baf10488d4526","last_reissued_at":"2026-05-18T01:11:21.173662Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:21.173662Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Neutrino Mass Generation and 750 GeV Diphoton excess via photon-photon fusion at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kirtiman Ghosh, S. Nandi, Sudip Jana","submitted_at":"2016-07-07T08:26:11Z","abstract_excerpt":"We propose a new model for explaining the diphoton excess observed at the LHC. The uniqueness of our model is that this excess is being produced by photon-photon induced sub-process. The model includes an isospin $3/2$ scalar multiplet (having triply, doubly and singly charged scalars) at the electroweak (EW) scale to explain the observed neutrino masses via the effective dimension $7$ operator. The model also include a singlet scalar which is the di-photon resonance. The loop induced coupling of the singlet scalar with a pair of photons is enhanced due to contributions from multi-charged EW-s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.01910","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":"1607.01910","created_at":"2026-05-18T01:11:21.173722+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.01910v2","created_at":"2026-05-18T01:11:21.173722+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.01910","created_at":"2026-05-18T01:11:21.173722+00:00"},{"alias_kind":"pith_short_12","alias_value":"IBUC5SA7CNGL","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_16","alias_value":"IBUC5SA7CNGLM7KL","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_8","alias_value":"IBUC5SA7","created_at":"2026-05-18T12:30:22.444734+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":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN","json":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN.json","graph_json":"https://pith.science/api/pith-number/IBUC5SA7CNGLM7KLDUUQPR2QUN/graph.json","events_json":"https://pith.science/api/pith-number/IBUC5SA7CNGLM7KLDUUQPR2QUN/events.json","paper":"https://pith.science/paper/IBUC5SA7"},"agent_actions":{"view_html":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN","download_json":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN.json","view_paper":"https://pith.science/paper/IBUC5SA7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.01910&json=true","fetch_graph":"https://pith.science/api/pith-number/IBUC5SA7CNGLM7KLDUUQPR2QUN/graph.json","fetch_events":"https://pith.science/api/pith-number/IBUC5SA7CNGLM7KLDUUQPR2QUN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN/action/storage_attestation","attest_author":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN/action/author_attestation","sign_citation":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN/action/citation_signature","submit_replication":"https://pith.science/pith/IBUC5SA7CNGLM7KLDUUQPR2QUN/action/replication_record"}},"created_at":"2026-05-18T01:11:21.173722+00:00","updated_at":"2026-05-18T01:11:21.173722+00:00"}