{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:QOBXSYTXY3KCMUNOVU2BNMYXFO","short_pith_number":"pith:QOBXSYTX","schema_version":"1.0","canonical_sha256":"8383796277c6d42651aead3416b3172bbd16bc0c6216dfed1a49164ac43b019d","source":{"kind":"arxiv","id":"2402.10503","version":2},"attestation_state":"computed","paper":{"title":"Automated resummation of electroweak Sudakov logarithms in diboson production at future colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ansgar Denner, Stefan Rode","submitted_at":"2024-02-16T08:24:09Z","abstract_excerpt":"At energies that are large with respect to the electroweak scale, the electroweak corrections to scattering processes involve large logarithms that have to be resummed to obtain decent predictions. Soft-collinear effective theory (SCET) has been proposed as a suitable framework to allow for this resummation, while retaining non-logarithmic corrections in a consistent way. In this paper, we investigate the approximations needed to use this approach for the calculation of electroweak corrections to off-shell diboson production at high-energy colliders. Upon implementing the method into a Monte-C"},"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":"2402.10503","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-02-16T08:24:09Z","cross_cats_sorted":[],"title_canon_sha256":"ab93e5525295cc9bd8a45d87dfed24de35971fafb2f4ea2a09d683cc2795cc94","abstract_canon_sha256":"eb6cc47c3a5171f0b36465414b7f6568cca3224531ff1724de8a63d9b94b3383"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:26:19.708580Z","signature_b64":"ap2/FPUpgnc70o23xl3r1hB0CV/OWIy0XMU57UeWHpHTMlXPqwjajUwB7kClhfOWF57dyZxOCj7fw7udz4+ICg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8383796277c6d42651aead3416b3172bbd16bc0c6216dfed1a49164ac43b019d","last_reissued_at":"2026-07-05T08:26:19.708101Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:26:19.708101Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Automated resummation of electroweak Sudakov logarithms in diboson production at future colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ansgar Denner, Stefan Rode","submitted_at":"2024-02-16T08:24:09Z","abstract_excerpt":"At energies that are large with respect to the electroweak scale, the electroweak corrections to scattering processes involve large logarithms that have to be resummed to obtain decent predictions. Soft-collinear effective theory (SCET) has been proposed as a suitable framework to allow for this resummation, while retaining non-logarithmic corrections in a consistent way. In this paper, we investigate the approximations needed to use this approach for the calculation of electroweak corrections to off-shell diboson production at high-energy colliders. Upon implementing the method into a Monte-C"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.10503","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/2402.10503/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":"2402.10503","created_at":"2026-07-05T08:26:19.708159+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.10503v2","created_at":"2026-07-05T08:26:19.708159+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.10503","created_at":"2026-07-05T08:26:19.708159+00:00"},{"alias_kind":"pith_short_12","alias_value":"QOBXSYTXY3KC","created_at":"2026-07-05T08:26:19.708159+00:00"},{"alias_kind":"pith_short_16","alias_value":"QOBXSYTXY3KCMUNO","created_at":"2026-07-05T08:26:19.708159+00:00"},{"alias_kind":"pith_short_8","alias_value":"QOBXSYTX","created_at":"2026-07-05T08:26:19.708159+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"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":76,"is_internal_anchor":false},{"citing_arxiv_id":"2605.28667","citing_title":"Towards the two-loop electroweak corrections to the Drell-Yan process: the complete fermionic contributions","ref_index":32,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14320","citing_title":"Logarithmic EW corrections at two-loop","ref_index":28,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO","json":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO.json","graph_json":"https://pith.science/api/pith-number/QOBXSYTXY3KCMUNOVU2BNMYXFO/graph.json","events_json":"https://pith.science/api/pith-number/QOBXSYTXY3KCMUNOVU2BNMYXFO/events.json","paper":"https://pith.science/paper/QOBXSYTX"},"agent_actions":{"view_html":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO","download_json":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO.json","view_paper":"https://pith.science/paper/QOBXSYTX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.10503&json=true","fetch_graph":"https://pith.science/api/pith-number/QOBXSYTXY3KCMUNOVU2BNMYXFO/graph.json","fetch_events":"https://pith.science/api/pith-number/QOBXSYTXY3KCMUNOVU2BNMYXFO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO/action/storage_attestation","attest_author":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO/action/author_attestation","sign_citation":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO/action/citation_signature","submit_replication":"https://pith.science/pith/QOBXSYTXY3KCMUNOVU2BNMYXFO/action/replication_record"}},"created_at":"2026-07-05T08:26:19.708159+00:00","updated_at":"2026-07-05T08:26:19.708159+00:00"}