{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:6VOCG6HSSKD5GNLXBSKY7UV7FZ","short_pith_number":"pith:6VOCG6HS","schema_version":"1.0","canonical_sha256":"f55c2378f29287d335770c958fd2bf2e629fbe783e89808872878a6bc94c6e88","source":{"kind":"arxiv","id":"2603.22233","version":2},"attestation_state":"computed","paper":{"title":"Search for Higgs boson production at high transverse momentum in the WW decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2026-03-23T17:29:09Z","abstract_excerpt":"A search for Higgs boson (H) production at high transverse momentum ($p_\\mathrm{T}$) in the WW decay channel is presented. The analysis uses proton-proton collisions at $\\sqrt{s}$ = 13 TeV recorded by the CMS experiment in 2016$-$2018, corresponding to an integrated luminosity of 138 fb$^{-1}$. The visible decay products of the Higgs boson are reconstructed as a single large-radius jet with one isolated lepton or none (1$\\ell$ and 0$\\ell$, respectively; $\\ell$ = e, $\\mu$). The H-candidate jets are identified using an advanced transformer-based algorithm and are calibrated with the Lund jet pla"},"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":"2603.22233","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-03-23T17:29:09Z","cross_cats_sorted":[],"title_canon_sha256":"ad88ef1dfc01aef062911b97a080ea373a028bec1e192878f04514840d48ef6b","abstract_canon_sha256":"b038f0c7d909c9ae89b3f98ffeefbb61523a554191999382e8e6b5a86ba73edd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-04T00:31:13.550678Z","signature_b64":"j1362WRR5RkCszb2YA0wAY1/RfHUZOoHWMxTA8oKKD+iQRaC+3rn2vhANMfz31GMEL89VURo1Soau0P6MkU1Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f55c2378f29287d335770c958fd2bf2e629fbe783e89808872878a6bc94c6e88","last_reissued_at":"2026-08-04T00:31:13.548961Z","signature_status":"signed_v1","first_computed_at":"2026-08-04T00:31:13.548961Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for Higgs boson production at high transverse momentum in the WW decay channel in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2026-03-23T17:29:09Z","abstract_excerpt":"A search for Higgs boson (H) production at high transverse momentum ($p_\\mathrm{T}$) in the WW decay channel is presented. The analysis uses proton-proton collisions at $\\sqrt{s}$ = 13 TeV recorded by the CMS experiment in 2016$-$2018, corresponding to an integrated luminosity of 138 fb$^{-1}$. The visible decay products of the Higgs boson are reconstructed as a single large-radius jet with one isolated lepton or none (1$\\ell$ and 0$\\ell$, respectively; $\\ell$ = e, $\\mu$). The H-candidate jets are identified using an advanced transformer-based algorithm and are calibrated with the Lund jet pla"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.22233","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/2603.22233/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":"2603.22233","created_at":"2026-08-04T00:31:13.550060+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.22233v2","created_at":"2026-08-04T00:31:13.550060+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.22233","created_at":"2026-08-04T00:31:13.550060+00:00"},{"alias_kind":"pith_short_12","alias_value":"6VOCG6HSSKD5","created_at":"2026-08-04T00:31:13.550060+00:00"},{"alias_kind":"pith_short_16","alias_value":"6VOCG6HSSKD5GNLX","created_at":"2026-08-04T00:31:13.550060+00:00"},{"alias_kind":"pith_short_8","alias_value":"6VOCG6HS","created_at":"2026-08-04T00:31:13.550060+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.26821","citing_title":"Particle-Lund Multimodality in Jet Taggers","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ","json":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ.json","graph_json":"https://pith.science/api/pith-number/6VOCG6HSSKD5GNLXBSKY7UV7FZ/graph.json","events_json":"https://pith.science/api/pith-number/6VOCG6HSSKD5GNLXBSKY7UV7FZ/events.json","paper":"https://pith.science/paper/6VOCG6HS"},"agent_actions":{"view_html":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ","download_json":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ.json","view_paper":"https://pith.science/paper/6VOCG6HS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.22233&json=true","fetch_graph":"https://pith.science/api/pith-number/6VOCG6HSSKD5GNLXBSKY7UV7FZ/graph.json","fetch_events":"https://pith.science/api/pith-number/6VOCG6HSSKD5GNLXBSKY7UV7FZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ/action/storage_attestation","attest_author":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ/action/author_attestation","sign_citation":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ/action/citation_signature","submit_replication":"https://pith.science/pith/6VOCG6HSSKD5GNLXBSKY7UV7FZ/action/replication_record"}},"created_at":"2026-08-04T00:31:13.550060+00:00","updated_at":"2026-08-04T00:31:13.550060+00:00"}