{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:PSBNTA3GATWWLICWAD3LA5CWLQ","short_pith_number":"pith:PSBNTA3G","schema_version":"1.0","canonical_sha256":"7c82d9836604ed65a05600f6b074565c2ee0732b36f3efeaa495b4e36a0690de","source":{"kind":"arxiv","id":"2008.12204","version":1},"attestation_state":"computed","paper":{"title":"Electroweak Couplings of the Higgs Boson at a Multi-TeV Muon Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Da Liu, Ian Low, Tao Han, Xing Wang","submitted_at":"2020-08-27T16:00:20Z","abstract_excerpt":"We estimate the expected precision at a multi-TeV muon collider for measuring the Higgs boson couplings with electroweak gauge bosons, $HVV$ and $HHVV\\ (V=W^\\pm,Z)$, as well as the trilinear Higgs self-coupling $HHH$. At very high energies both single and double Higgs productions rely on the vector-boson fusion (VBF) topology. The outgoing remnant particles have a strong tendency to stay in the very forward region, leading to the configuration of the \"inclusive process\" and making it difficult to isolate $ZZ$ fusion events from the $WW$ fusion. In the single Higgs channel, we perform a maximum"},"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":"2008.12204","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-08-27T16:00:20Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"9b5a85c2904965fb794bfe2222959f3bbfd596ba1a33a7c011b29740cf154490","abstract_canon_sha256":"ea7372736132a61a3ecb4f39acdd8b4475a38a27b6eb246e9bfc287f6e1a771d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:06:12.431323Z","signature_b64":"Fhxk+S9TB+Hwqv2POGmuGzf2GU+iA7BP0HfiI/XlJBzlUnwcjNWK9PG5VOa0rYJzGkncJHzHdFCrgPowxDRJBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c82d9836604ed65a05600f6b074565c2ee0732b36f3efeaa495b4e36a0690de","last_reissued_at":"2026-07-05T02:06:12.430851Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:06:12.430851Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electroweak Couplings of the Higgs Boson at a Multi-TeV Muon Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Da Liu, Ian Low, Tao Han, Xing Wang","submitted_at":"2020-08-27T16:00:20Z","abstract_excerpt":"We estimate the expected precision at a multi-TeV muon collider for measuring the Higgs boson couplings with electroweak gauge bosons, $HVV$ and $HHVV\\ (V=W^\\pm,Z)$, as well as the trilinear Higgs self-coupling $HHH$. At very high energies both single and double Higgs productions rely on the vector-boson fusion (VBF) topology. The outgoing remnant particles have a strong tendency to stay in the very forward region, leading to the configuration of the \"inclusive process\" and making it difficult to isolate $ZZ$ fusion events from the $WW$ fusion. In the single Higgs channel, we perform a maximum"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2008.12204","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/2008.12204/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":"2008.12204","created_at":"2026-07-05T02:06:12.430907+00:00"},{"alias_kind":"arxiv_version","alias_value":"2008.12204v1","created_at":"2026-07-05T02:06:12.430907+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2008.12204","created_at":"2026-07-05T02:06:12.430907+00:00"},{"alias_kind":"pith_short_12","alias_value":"PSBNTA3GATWW","created_at":"2026-07-05T02:06:12.430907+00:00"},{"alias_kind":"pith_short_16","alias_value":"PSBNTA3GATWWLICW","created_at":"2026-07-05T02:06:12.430907+00:00"},{"alias_kind":"pith_short_8","alias_value":"PSBNTA3G","created_at":"2026-07-05T02:06:12.430907+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.07746","citing_title":"Dark Z' at a Muon Collider: Radiative Return versus Vector Boson Fusion","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2411.00096","citing_title":"Why detect forward muons at a muon collider","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13957","citing_title":"Heavy Vector Triplets at a Muon Collider","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08688","citing_title":"Probing Higgs and Top Interactions through the Muon Lens at multi-TeV Muon Colliders","ref_index":17,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ","json":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ.json","graph_json":"https://pith.science/api/pith-number/PSBNTA3GATWWLICWAD3LA5CWLQ/graph.json","events_json":"https://pith.science/api/pith-number/PSBNTA3GATWWLICWAD3LA5CWLQ/events.json","paper":"https://pith.science/paper/PSBNTA3G"},"agent_actions":{"view_html":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ","download_json":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ.json","view_paper":"https://pith.science/paper/PSBNTA3G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2008.12204&json=true","fetch_graph":"https://pith.science/api/pith-number/PSBNTA3GATWWLICWAD3LA5CWLQ/graph.json","fetch_events":"https://pith.science/api/pith-number/PSBNTA3GATWWLICWAD3LA5CWLQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ/action/storage_attestation","attest_author":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ/action/author_attestation","sign_citation":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ/action/citation_signature","submit_replication":"https://pith.science/pith/PSBNTA3GATWWLICWAD3LA5CWLQ/action/replication_record"}},"created_at":"2026-07-05T02:06:12.430907+00:00","updated_at":"2026-07-05T02:06:12.430907+00:00"}