{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:3B36NPAQAMOJ7TLH3UDWPK5SU5","short_pith_number":"pith:3B36NPAQ","schema_version":"1.0","canonical_sha256":"d877e6bc10031c9fcd67dd0767abb2a75245838aeec29ee76cd54cf0a6b0e246","source":{"kind":"arxiv","id":"1004.2188","version":1},"attestation_state":"computed","paper":{"title":"Electroweak non-resonant NLO corrections to e+ e- -> W+ W- b bbar in the t tbar resonance region","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Jantzen, M. Beneke, P. Ruiz-Femenia (RWTH Aachen University)","submitted_at":"2010-04-13T13:50:35Z","abstract_excerpt":"We analyse subleading electroweak effects in the top anti-top resonance production region in e+ e- collisions which arise due to the decay of the top and anti-top quarks into the W+ W- b bbar final state. These are NLO corrections adopting the non-relativistic power counting v ~ alpha_s ~ sqrt(alpha_EW). In contrast to the QCD corrections which have been calculated (almost) up to NNNLO, the parametrically larger NLO electroweak contributions have not been completely known so far, but are mandatory for the required accuracy at a future linear collider. The missing parts of these NLO contributio"},"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":"1004.2188","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-13T13:50:35Z","cross_cats_sorted":[],"title_canon_sha256":"a116eed123577ca8c26056a6fb87a4f47ca2bf3a059126527d31631603032539","abstract_canon_sha256":"3ea8846723f125539248bd972f11d573fb65d08e1542b922317c6972d63b7346"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:42:01.782186Z","signature_b64":"4QPMPC8ulyXMLHFabRfhC3vbXLkgF7YoiRzYgWzAQEgjpWMcn1GO39qt4sq2WYX0Sh73NnDrYQdYI5EtylbvCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d877e6bc10031c9fcd67dd0767abb2a75245838aeec29ee76cd54cf0a6b0e246","last_reissued_at":"2026-05-18T04:42:01.781838Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:42:01.781838Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electroweak non-resonant NLO corrections to e+ e- -> W+ W- b bbar in the t tbar resonance region","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. Jantzen, M. Beneke, P. Ruiz-Femenia (RWTH Aachen University)","submitted_at":"2010-04-13T13:50:35Z","abstract_excerpt":"We analyse subleading electroweak effects in the top anti-top resonance production region in e+ e- collisions which arise due to the decay of the top and anti-top quarks into the W+ W- b bbar final state. These are NLO corrections adopting the non-relativistic power counting v ~ alpha_s ~ sqrt(alpha_EW). In contrast to the QCD corrections which have been calculated (almost) up to NNNLO, the parametrically larger NLO electroweak contributions have not been completely known so far, but are mandatory for the required accuracy at a future linear collider. The missing parts of these NLO contributio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.2188","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":""},"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":"1004.2188","created_at":"2026-05-18T04:42:01.781893+00:00"},{"alias_kind":"arxiv_version","alias_value":"1004.2188v1","created_at":"2026-05-18T04:42:01.781893+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.2188","created_at":"2026-05-18T04:42:01.781893+00:00"},{"alias_kind":"pith_short_12","alias_value":"3B36NPAQAMOJ","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_16","alias_value":"3B36NPAQAMOJ7TLH","created_at":"2026-05-18T12:26:03.138858+00:00"},{"alias_kind":"pith_short_8","alias_value":"3B36NPAQ","created_at":"2026-05-18T12:26:03.138858+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.02179","citing_title":"Invariant-mass distribution of top-quark pairs and top-quark mass determination","ref_index":29,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5","json":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5.json","graph_json":"https://pith.science/api/pith-number/3B36NPAQAMOJ7TLH3UDWPK5SU5/graph.json","events_json":"https://pith.science/api/pith-number/3B36NPAQAMOJ7TLH3UDWPK5SU5/events.json","paper":"https://pith.science/paper/3B36NPAQ"},"agent_actions":{"view_html":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5","download_json":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5.json","view_paper":"https://pith.science/paper/3B36NPAQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1004.2188&json=true","fetch_graph":"https://pith.science/api/pith-number/3B36NPAQAMOJ7TLH3UDWPK5SU5/graph.json","fetch_events":"https://pith.science/api/pith-number/3B36NPAQAMOJ7TLH3UDWPK5SU5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5/action/storage_attestation","attest_author":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5/action/author_attestation","sign_citation":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5/action/citation_signature","submit_replication":"https://pith.science/pith/3B36NPAQAMOJ7TLH3UDWPK5SU5/action/replication_record"}},"created_at":"2026-05-18T04:42:01.781893+00:00","updated_at":"2026-05-18T04:42:01.781893+00:00"}