{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:S3GISMXC624RRHFBF7CGZSIFIS","short_pith_number":"pith:S3GISMXC","schema_version":"1.0","canonical_sha256":"96cc8932e2f6b9189ca12fc46cc90544ab6c4ba518017d5e319413197ab70d38","source":{"kind":"arxiv","id":"2503.19420","version":2},"attestation_state":"computed","paper":{"title":"Measurements of the production cross-sections of a Higgs boson in association with a vector boson and decaying into $WW^\\ast$ with the ATLAS detector at $\\sqrt{s} = 13$ TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2025-03-25T07:57:35Z","abstract_excerpt":"Measurements of the total and differential Higgs boson production cross-sections, via $WH$ and $ZH$ associated production using $H\\rightarrow WW^\\ast\\rightarrow\\ell\\nu\\ell\\nu$ and $H\\rightarrow WW^\\ast\\rightarrow\\ell\\nu jj$ decays, are presented. The analysis uses proton-proton events delivered by the Large Hadron Collider at a centre-of-mass energy of 13 TeV and recorded by the ATLAS detector between 2015 and 2018. The data correspond to an integrated luminosity of 140 fb$^{-1}$. The sum of the $WH$ and $ZH$ cross-sections times the $H\\rightarrow WW^\\ast$ branching fraction is measured to be "},"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":"2503.19420","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2025-03-25T07:57:35Z","cross_cats_sorted":[],"title_canon_sha256":"c3fdf9d7010956d0d30256cf257e4be6c8f307bc97e550d2d756a6bb3d23ec9b","abstract_canon_sha256":"c4070371d5ebeedcafe167eb60ad342879e1fffbd3b06ce336707a34c408a111"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:53:45.082192Z","signature_b64":"XL38bzFAqyQd31xMdj+yB/0X7QWIIyniok8/ps+VIgdnXx1uHfPEdRdqskdYNlM8/py5xHuI6Q4186IuMAj2Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"96cc8932e2f6b9189ca12fc46cc90544ab6c4ba518017d5e319413197ab70d38","last_reissued_at":"2026-07-05T11:53:45.081659Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:53:45.081659Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of the production cross-sections of a Higgs boson in association with a vector boson and decaying into $WW^\\ast$ with the ATLAS detector at $\\sqrt{s} = 13$ TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2025-03-25T07:57:35Z","abstract_excerpt":"Measurements of the total and differential Higgs boson production cross-sections, via $WH$ and $ZH$ associated production using $H\\rightarrow WW^\\ast\\rightarrow\\ell\\nu\\ell\\nu$ and $H\\rightarrow WW^\\ast\\rightarrow\\ell\\nu jj$ decays, are presented. The analysis uses proton-proton events delivered by the Large Hadron Collider at a centre-of-mass energy of 13 TeV and recorded by the ATLAS detector between 2015 and 2018. The data correspond to an integrated luminosity of 140 fb$^{-1}$. The sum of the $WH$ and $ZH$ cross-sections times the $H\\rightarrow WW^\\ast$ branching fraction is measured to be "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.19420","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2503.19420/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":"2503.19420","created_at":"2026-07-05T11:53:45.081713+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.19420v2","created_at":"2026-07-05T11:53:45.081713+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.19420","created_at":"2026-07-05T11:53:45.081713+00:00"},{"alias_kind":"pith_short_12","alias_value":"S3GISMXC624R","created_at":"2026-07-05T11:53:45.081713+00:00"},{"alias_kind":"pith_short_16","alias_value":"S3GISMXC624RRHFB","created_at":"2026-07-05T11:53:45.081713+00:00"},{"alias_kind":"pith_short_8","alias_value":"S3GISMXC","created_at":"2026-07-05T11:53:45.081713+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.01760","citing_title":"HS3: A Descriptive, Interoperable Serialization Standard for Statistical Models in High-Energy Physics","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS","json":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS.json","graph_json":"https://pith.science/api/pith-number/S3GISMXC624RRHFBF7CGZSIFIS/graph.json","events_json":"https://pith.science/api/pith-number/S3GISMXC624RRHFBF7CGZSIFIS/events.json","paper":"https://pith.science/paper/S3GISMXC"},"agent_actions":{"view_html":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS","download_json":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS.json","view_paper":"https://pith.science/paper/S3GISMXC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.19420&json=true","fetch_graph":"https://pith.science/api/pith-number/S3GISMXC624RRHFBF7CGZSIFIS/graph.json","fetch_events":"https://pith.science/api/pith-number/S3GISMXC624RRHFBF7CGZSIFIS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS/action/storage_attestation","attest_author":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS/action/author_attestation","sign_citation":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS/action/citation_signature","submit_replication":"https://pith.science/pith/S3GISMXC624RRHFBF7CGZSIFIS/action/replication_record"}},"created_at":"2026-07-05T11:53:45.081713+00:00","updated_at":"2026-07-05T11:53:45.081713+00:00"}