{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:33UBUYBRDVVK5RZLINWR7I6JIN","short_pith_number":"pith:33UBUYBR","schema_version":"1.0","canonical_sha256":"dee81a60311d6aaec72b436d1fa3c9435f500891c7548076ea74ab613e615972","source":{"kind":"arxiv","id":"2410.11140","version":1},"attestation_state":"computed","paper":{"title":"Unified Interpretation of 95 GeV Excesses in the Two Higgs Doublet type II Seesaw Model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Brahim Ait-Ouazghour, Khalid Goure, Mohamed Chabab","submitted_at":"2024-10-14T23:32:54Z","abstract_excerpt":"In the search for a light Higgs boson, the ATLAS and CMS experiments have observed excesses in both the diphoton ($\\gamma\\gamma$) and di-tau-pair ($\\tau^+\\tau^-$) decay channels at about $95$ GeV. The LEP collaboration has also previously reported an excess in the $b\\bar{b}$ channel at a comparable Higgs mass. In this paper, we explore whether these excesses can be accommodated within the framework of the Two Higgs Doublet type II Seesaw Model (2HDMcT). By implementing various theoretical constraints and experimental limits on the parameter space, we first demonstrate that a light CP-even Higg"},"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":"2410.11140","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-10-14T23:32:54Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f0fc7fc989f1365ce5712d638f376528443efce4a0c25c6bd81a60a87cd7fe3b","abstract_canon_sha256":"8be47942e7a11a301104dc0bade76a54ec04b880353ecaabb6596ae6e88d6795"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:20:29.811406Z","signature_b64":"ncbrvRBvtisE7IbNJy+4Cjx821gO2b+Lk93sATVeiboH9Xt0HcyvS7hx15JFu0kfsvNzNF6dI14RnX6g/hSWCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dee81a60311d6aaec72b436d1fa3c9435f500891c7548076ea74ab613e615972","last_reissued_at":"2026-07-05T09:20:29.810950Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:20:29.810950Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unified Interpretation of 95 GeV Excesses in the Two Higgs Doublet type II Seesaw Model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Brahim Ait-Ouazghour, Khalid Goure, Mohamed Chabab","submitted_at":"2024-10-14T23:32:54Z","abstract_excerpt":"In the search for a light Higgs boson, the ATLAS and CMS experiments have observed excesses in both the diphoton ($\\gamma\\gamma$) and di-tau-pair ($\\tau^+\\tau^-$) decay channels at about $95$ GeV. The LEP collaboration has also previously reported an excess in the $b\\bar{b}$ channel at a comparable Higgs mass. In this paper, we explore whether these excesses can be accommodated within the framework of the Two Higgs Doublet type II Seesaw Model (2HDMcT). By implementing various theoretical constraints and experimental limits on the parameter space, we first demonstrate that a light CP-even Higg"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.11140","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/2410.11140/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":"2410.11140","created_at":"2026-07-05T09:20:29.811012+00:00"},{"alias_kind":"arxiv_version","alias_value":"2410.11140v1","created_at":"2026-07-05T09:20:29.811012+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.11140","created_at":"2026-07-05T09:20:29.811012+00:00"},{"alias_kind":"pith_short_12","alias_value":"33UBUYBRDVVK","created_at":"2026-07-05T09:20:29.811012+00:00"},{"alias_kind":"pith_short_16","alias_value":"33UBUYBRDVVK5RZL","created_at":"2026-07-05T09:20:29.811012+00:00"},{"alias_kind":"pith_short_8","alias_value":"33UBUYBR","created_at":"2026-07-05T09:20:29.811012+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.04493","citing_title":"A comprehensive study of the charged Higgs boson in the two Higgs doublet type-II seesaw model","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN","json":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN.json","graph_json":"https://pith.science/api/pith-number/33UBUYBRDVVK5RZLINWR7I6JIN/graph.json","events_json":"https://pith.science/api/pith-number/33UBUYBRDVVK5RZLINWR7I6JIN/events.json","paper":"https://pith.science/paper/33UBUYBR"},"agent_actions":{"view_html":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN","download_json":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN.json","view_paper":"https://pith.science/paper/33UBUYBR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2410.11140&json=true","fetch_graph":"https://pith.science/api/pith-number/33UBUYBRDVVK5RZLINWR7I6JIN/graph.json","fetch_events":"https://pith.science/api/pith-number/33UBUYBRDVVK5RZLINWR7I6JIN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN/action/storage_attestation","attest_author":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN/action/author_attestation","sign_citation":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN/action/citation_signature","submit_replication":"https://pith.science/pith/33UBUYBRDVVK5RZLINWR7I6JIN/action/replication_record"}},"created_at":"2026-07-05T09:20:29.811012+00:00","updated_at":"2026-07-05T09:20:29.811012+00:00"}