{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:WC4INZGZ6NJPUG74EJOC7EZ52J","short_pith_number":"pith:WC4INZGZ","schema_version":"1.0","canonical_sha256":"b0b886e4d9f352fa1bfc225c2f933dd270cf76887db8cf17f238485caac6ffcb","source":{"kind":"arxiv","id":"2409.03620","version":2},"attestation_state":"computed","paper":{"title":"NLO EW and QCD corrections to polarised same-sign WW scattering at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ansgar Denner, Christoph Haitz, Giovanni Pelliccioli","submitted_at":"2024-09-05T15:26:44Z","abstract_excerpt":"We present the first calculation of same-sign WW scattering at the LHC in the fully leptonic decay channel including the modelling of polarisation for intermediate electroweak bosons and radiative corrections up to NLO EW+QCD accuracy. The predictions rely on a pole expansion and on the split of polarisation states at matrix-element level. Doubly-polarised and unpolarised signals are investigated together with full off-shell results. A detailed phenomenlogical analysis is carried out focusing on differential observables that discriminate between polarisation states, paving the way for refined "},"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":"2409.03620","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-09-05T15:26:44Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3f81cd2317e1a058e4262b6f53109abeb78adb65b971a84beb48722198702a50","abstract_canon_sha256":"8b61dfa788669fd8b788f2c1780fa4c173592dd364ba6c53d0603bdae685f4e6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:34:18.587135Z","signature_b64":"ZR/MNCqJe7I/nvhKxQlhQnMJeGhFmfCF2nIp0fW7rrxlWK7t7QM120Dt9Mx6pKQ/PnBAV59DoS3cqDgFU6zzCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b0b886e4d9f352fa1bfc225c2f933dd270cf76887db8cf17f238485caac6ffcb","last_reissued_at":"2026-07-05T09:34:18.586684Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:34:18.586684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"NLO EW and QCD corrections to polarised same-sign WW scattering at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Ansgar Denner, Christoph Haitz, Giovanni Pelliccioli","submitted_at":"2024-09-05T15:26:44Z","abstract_excerpt":"We present the first calculation of same-sign WW scattering at the LHC in the fully leptonic decay channel including the modelling of polarisation for intermediate electroweak bosons and radiative corrections up to NLO EW+QCD accuracy. The predictions rely on a pole expansion and on the split of polarisation states at matrix-element level. Doubly-polarised and unpolarised signals are investigated together with full off-shell results. A detailed phenomenlogical analysis is carried out focusing on differential observables that discriminate between polarisation states, paving the way for refined "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2409.03620","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/2409.03620/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":"2409.03620","created_at":"2026-07-05T09:34:18.586744+00:00"},{"alias_kind":"arxiv_version","alias_value":"2409.03620v2","created_at":"2026-07-05T09:34:18.586744+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2409.03620","created_at":"2026-07-05T09:34:18.586744+00:00"},{"alias_kind":"pith_short_12","alias_value":"WC4INZGZ6NJP","created_at":"2026-07-05T09:34:18.586744+00:00"},{"alias_kind":"pith_short_16","alias_value":"WC4INZGZ6NJPUG74","created_at":"2026-07-05T09:34:18.586744+00:00"},{"alias_kind":"pith_short_8","alias_value":"WC4INZGZ","created_at":"2026-07-05T09:34:18.586744+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19999","citing_title":"NLO QCD and EW corrections to semileptonic vector-boson scattering at the LHC","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2606.11296","citing_title":"Tripartite Entanglement in $e^+ e^- \\to t \\bar{t} Z$","ref_index":92,"is_internal_anchor":false},{"citing_arxiv_id":"2606.06436","citing_title":"Probing anomalous quartic gauge couplings in same-sign $W$ boson scattering with polarization and spin correlation","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2607.00962","citing_title":"Higher-order effects in amplitude-assisted polarisation extraction with machine-learning techniques","ref_index":16,"is_internal_anchor":false},{"citing_arxiv_id":"2607.01174","citing_title":"The cleanest of them all: NLO electroweak corrections to vector-boson scattering into doubly polarised ZZ pairs at the LHC","ref_index":19,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16218","citing_title":"Quantum Tomography and Entanglement in Semi-Leptonic $h\\to VV^*$ Decays at Higher Orders","ref_index":90,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J","json":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J.json","graph_json":"https://pith.science/api/pith-number/WC4INZGZ6NJPUG74EJOC7EZ52J/graph.json","events_json":"https://pith.science/api/pith-number/WC4INZGZ6NJPUG74EJOC7EZ52J/events.json","paper":"https://pith.science/paper/WC4INZGZ"},"agent_actions":{"view_html":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J","download_json":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J.json","view_paper":"https://pith.science/paper/WC4INZGZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2409.03620&json=true","fetch_graph":"https://pith.science/api/pith-number/WC4INZGZ6NJPUG74EJOC7EZ52J/graph.json","fetch_events":"https://pith.science/api/pith-number/WC4INZGZ6NJPUG74EJOC7EZ52J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J/action/storage_attestation","attest_author":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J/action/author_attestation","sign_citation":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J/action/citation_signature","submit_replication":"https://pith.science/pith/WC4INZGZ6NJPUG74EJOC7EZ52J/action/replication_record"}},"created_at":"2026-07-05T09:34:18.586744+00:00","updated_at":"2026-07-05T09:34:18.586744+00:00"}