{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:KSRMMLZ3GVZ6VXOS6BLBY2WSSY","short_pith_number":"pith:KSRMMLZ3","schema_version":"1.0","canonical_sha256":"54a2c62f3b3573eaddd2f0561c6ad2962eab1ec35802d6af1d5dea58f67c7d05","source":{"kind":"arxiv","id":"1003.3926","version":1},"attestation_state":"computed","paper":{"title":"Distributions and correlations for top quark pair production and decay at the Tevatron and LHC.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Werner Bernreuther, Zong-Guo Si","submitted_at":"2010-03-20T12:27:05Z","abstract_excerpt":"We investigate a number of  observables  that are and will be instrumental in the exploration of $\\tbart$ production and decay at the Tevatron and the LHC. For this analysis we made a computer program that incorporates besides the NLO QCD corrections to $\\tbart$ production and decay also mixed weak-QCD corrections to the production amplitudes, and that allows for studies of correlated versus uncorrelated $\\tbart$ events. In this paper we analyze and compute observables mostly for dileptonic $\\tbart$ final states to next-to-leading order in the strong and weak gauge couplings (NLOW), with selec"},"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":"1003.3926","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-03-20T12:27:05Z","cross_cats_sorted":[],"title_canon_sha256":"734b821d222870cc4bf545551b03a7080ff1317a5e90bef235ddeedd4b714d3a","abstract_canon_sha256":"d077727cfc98bfd11b4e81956aa8ab8eaf3b457323b7705f92c91684e954a6e1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:40.710966Z","signature_b64":"lKl+c3rJsG466Jf8vgoZm7ZG2vm4H/4ASH3hrqjgntjAszMaYJFQPtebJr8VQjHFaeQY+eyuPdfyZs4J6RRhBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"54a2c62f3b3573eaddd2f0561c6ad2962eab1ec35802d6af1d5dea58f67c7d05","last_reissued_at":"2026-05-18T02:33:40.710504Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:40.710504Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Distributions and correlations for top quark pair production and decay at the Tevatron and LHC.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Werner Bernreuther, Zong-Guo Si","submitted_at":"2010-03-20T12:27:05Z","abstract_excerpt":"We investigate a number of  observables  that are and will be instrumental in the exploration of $\\tbart$ production and decay at the Tevatron and the LHC. For this analysis we made a computer program that incorporates besides the NLO QCD corrections to $\\tbart$ production and decay also mixed weak-QCD corrections to the production amplitudes, and that allows for studies of correlated versus uncorrelated $\\tbart$ events. In this paper we analyze and compute observables mostly for dileptonic $\\tbart$ final states to next-to-leading order in the strong and weak gauge couplings (NLOW), with selec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.3926","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":"1003.3926","created_at":"2026-05-18T02:33:40.710590+00:00"},{"alias_kind":"arxiv_version","alias_value":"1003.3926v1","created_at":"2026-05-18T02:33:40.710590+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.3926","created_at":"2026-05-18T02:33:40.710590+00:00"},{"alias_kind":"pith_short_12","alias_value":"KSRMMLZ3GVZ6","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"KSRMMLZ3GVZ6VXOS","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"KSRMMLZ3","created_at":"2026-05-18T12:26:09.077623+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.07585","citing_title":"Particle Collisions & Quantum Entanglement in High-Energy Collisions","ref_index":103,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY","json":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY.json","graph_json":"https://pith.science/api/pith-number/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/graph.json","events_json":"https://pith.science/api/pith-number/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/events.json","paper":"https://pith.science/paper/KSRMMLZ3"},"agent_actions":{"view_html":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY","download_json":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY.json","view_paper":"https://pith.science/paper/KSRMMLZ3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1003.3926&json=true","fetch_graph":"https://pith.science/api/pith-number/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/graph.json","fetch_events":"https://pith.science/api/pith-number/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/action/storage_attestation","attest_author":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/action/author_attestation","sign_citation":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/action/citation_signature","submit_replication":"https://pith.science/pith/KSRMMLZ3GVZ6VXOS6BLBY2WSSY/action/replication_record"}},"created_at":"2026-05-18T02:33:40.710590+00:00","updated_at":"2026-05-18T02:33:40.710590+00:00"}