{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:EYURU3C6Z7QLMAAMTWWRERRLAA","short_pith_number":"pith:EYURU3C6","schema_version":"1.0","canonical_sha256":"26291a6c5ecfe0b6000c9dad12462b000460b437a6f3010e6aaf49facae0a4e9","source":{"kind":"arxiv","id":"2503.13719","version":3},"attestation_state":"computed","paper":{"title":"The Higgs Self-Coupling at FCC-ee","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ben A. Stefanek, Tevong You, Victor Maura","submitted_at":"2025-03-17T20:56:57Z","abstract_excerpt":"Single Higgs production at FCC-ee probes the Higgs self-coupling at next-to-leading order (NLO). Extracting a bound requires a global analysis accounting for other possible new physics contributions up to NLO. We determine the FCC-ee sensitivity to Higgs self-coupling modifications $\\delta\\kappa_\\lambda$ within the Standard Model Effective Field Theory (SMEFT) framework, including for the first time flavour, LEP, LHC, and FCC-ee observables in a global analysis with all leading NLO effects via one-loop renormalisation group evolution, as well as incorporating finite NLO contributions to electr"},"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":"2503.13719","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-03-17T20:56:57Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"fb8032d7d74a0b0c14f74afaec9cadd3933a65bb998e75230777878196bc121e","abstract_canon_sha256":"a15df9a3824b4094c7d843a50653b115afb0df3d6b77b5a009265b22452fe253"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:49:52.367016Z","signature_b64":"kDMgrSMNWMvJz97gnQnfmZlQg8fxmAo54juU/JAvjKz9drUjcD3KtuBAO3n+Ldbp3FpGfzIGg7472GWx+DJSBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"26291a6c5ecfe0b6000c9dad12462b000460b437a6f3010e6aaf49facae0a4e9","last_reissued_at":"2026-07-05T10:49:52.366515Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:49:52.366515Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Higgs Self-Coupling at FCC-ee","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ben A. Stefanek, Tevong You, Victor Maura","submitted_at":"2025-03-17T20:56:57Z","abstract_excerpt":"Single Higgs production at FCC-ee probes the Higgs self-coupling at next-to-leading order (NLO). Extracting a bound requires a global analysis accounting for other possible new physics contributions up to NLO. We determine the FCC-ee sensitivity to Higgs self-coupling modifications $\\delta\\kappa_\\lambda$ within the Standard Model Effective Field Theory (SMEFT) framework, including for the first time flavour, LEP, LHC, and FCC-ee observables in a global analysis with all leading NLO effects via one-loop renormalisation group evolution, as well as incorporating finite NLO contributions to electr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.13719","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/2503.13719/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":"2503.13719","created_at":"2026-07-05T10:49:52.366573+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.13719v3","created_at":"2026-07-05T10:49:52.366573+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.13719","created_at":"2026-07-05T10:49:52.366573+00:00"},{"alias_kind":"pith_short_12","alias_value":"EYURU3C6Z7QL","created_at":"2026-07-05T10:49:52.366573+00:00"},{"alias_kind":"pith_short_16","alias_value":"EYURU3C6Z7QLMAAM","created_at":"2026-07-05T10:49:52.366573+00:00"},{"alias_kind":"pith_short_8","alias_value":"EYURU3C6","created_at":"2026-07-05T10:49:52.366573+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.21594","citing_title":"Exploring the SMEFT landscape: Bayesian Model Selection for indirect discovery","ref_index":32,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24152","citing_title":"Probing the electron Yukawa coupling via resonant Higgs boson production at FCC-ee via $e^+e^- \\to H \\to WW^*$ in lepton-plus-jets final states","ref_index":17,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14284","citing_title":"A Busy Higgs Signal","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA","json":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA.json","graph_json":"https://pith.science/api/pith-number/EYURU3C6Z7QLMAAMTWWRERRLAA/graph.json","events_json":"https://pith.science/api/pith-number/EYURU3C6Z7QLMAAMTWWRERRLAA/events.json","paper":"https://pith.science/paper/EYURU3C6"},"agent_actions":{"view_html":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA","download_json":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA.json","view_paper":"https://pith.science/paper/EYURU3C6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.13719&json=true","fetch_graph":"https://pith.science/api/pith-number/EYURU3C6Z7QLMAAMTWWRERRLAA/graph.json","fetch_events":"https://pith.science/api/pith-number/EYURU3C6Z7QLMAAMTWWRERRLAA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA/action/storage_attestation","attest_author":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA/action/author_attestation","sign_citation":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA/action/citation_signature","submit_replication":"https://pith.science/pith/EYURU3C6Z7QLMAAMTWWRERRLAA/action/replication_record"}},"created_at":"2026-07-05T10:49:52.366573+00:00","updated_at":"2026-07-05T10:49:52.366573+00:00"}