{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:4BKD3TQFKOTW5VVAPHS2STA7GR","short_pith_number":"pith:4BKD3TQF","schema_version":"1.0","canonical_sha256":"e0543dce0553a76ed6a079e5a94c1f34453fcc92359e6232c67d21bb4a964c16","source":{"kind":"arxiv","id":"hep-ex/0309076","version":1},"attestation_state":"computed","paper":{"title":"Search for Doubly-Charged Higgs Bosons at LEP","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"L3 Collaboration","submitted_at":"2003-09-26T15:01:46Z","abstract_excerpt":"Doubly-charged Higgs bosons are searched for in e^+e^- collision data collected with the L3 detector at LEP at centre-of-mass energies up to 209 GeV. Final states with four leptons are analysed to tag the pair-production of doubly charged Higgs bosons. No significant excess is found and lower limits at 95% confidence level on the doubly-charged Higgs boson mass are derived. They vary from 95.5 GeV to 100.2 GeV, depending on the decay mode. Doubly-charged Higgs bosons which couple to electrons would modify the cross section and forward-backward asymmetry of the e^+e^- -> e^+e^- process. The mea"},"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":"hep-ex/0309076","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2003-09-26T15:01:46Z","cross_cats_sorted":[],"title_canon_sha256":"89f5266e1056a9903a4c98f63bc3de471f73e5f01376bee080aea189a7526572","abstract_canon_sha256":"3c5c969ae0d59e703e382da3bc5f11990eedb46457ff6041bd3b5ef3abd29a00"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:31.737701Z","signature_b64":"YHMeP2nFDT3o+1mCmEBBHb46uLMWcLxpjuhNzs7IVyp9ICDH7x69UJTa8cGigHvjjtciezGQCXVvqzhsRPmQCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e0543dce0553a76ed6a079e5a94c1f34453fcc92359e6232c67d21bb4a964c16","last_reissued_at":"2026-05-18T03:47:31.736877Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:31.736877Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for Doubly-Charged Higgs Bosons at LEP","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"L3 Collaboration","submitted_at":"2003-09-26T15:01:46Z","abstract_excerpt":"Doubly-charged Higgs bosons are searched for in e^+e^- collision data collected with the L3 detector at LEP at centre-of-mass energies up to 209 GeV. Final states with four leptons are analysed to tag the pair-production of doubly charged Higgs bosons. No significant excess is found and lower limits at 95% confidence level on the doubly-charged Higgs boson mass are derived. They vary from 95.5 GeV to 100.2 GeV, depending on the decay mode. Doubly-charged Higgs bosons which couple to electrons would modify the cross section and forward-backward asymmetry of the e^+e^- -> e^+e^- process. The mea"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0309076","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":"hep-ex/0309076","created_at":"2026-05-18T03:47:31.737017+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0309076v1","created_at":"2026-05-18T03:47:31.737017+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0309076","created_at":"2026-05-18T03:47:31.737017+00:00"},{"alias_kind":"pith_short_12","alias_value":"4BKD3TQFKOTW","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"4BKD3TQFKOTW5VVA","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"4BKD3TQF","created_at":"2026-05-18T12:25:51.375804+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.29031","citing_title":"Twilight of the WIMP: Comprehensive Phenomenology of Electroweak Triplet Dark Matter","ref_index":51,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR","json":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR.json","graph_json":"https://pith.science/api/pith-number/4BKD3TQFKOTW5VVAPHS2STA7GR/graph.json","events_json":"https://pith.science/api/pith-number/4BKD3TQFKOTW5VVAPHS2STA7GR/events.json","paper":"https://pith.science/paper/4BKD3TQF"},"agent_actions":{"view_html":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR","download_json":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR.json","view_paper":"https://pith.science/paper/4BKD3TQF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0309076&json=true","fetch_graph":"https://pith.science/api/pith-number/4BKD3TQFKOTW5VVAPHS2STA7GR/graph.json","fetch_events":"https://pith.science/api/pith-number/4BKD3TQFKOTW5VVAPHS2STA7GR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR/action/storage_attestation","attest_author":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR/action/author_attestation","sign_citation":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR/action/citation_signature","submit_replication":"https://pith.science/pith/4BKD3TQFKOTW5VVAPHS2STA7GR/action/replication_record"}},"created_at":"2026-05-18T03:47:31.737017+00:00","updated_at":"2026-05-18T03:47:31.737017+00:00"}