{"doi":"10.1103/physrevd.67.071503","title":"Next-to-leading order QCD corrections to<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>p</mml:mi><mml:mrow><mml:mrow><mml:mover><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mo>→</mml:mo></mml:mrow></mml:mover></mml:mrow></mml:mrow><mml:mi>t</mml:mi><mml:mrow><mml:mrow><mml:mover><mml:mrow><mml:mi>t</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:mover></mml:mrow></mml:mrow><mml:mi>h</mml:mi></mml:math>at the CERN Large Hadron Collider","abstract":"We compute the $\\mathcal{O}({\\ensuremath{\\alpha}}_{s}^{3})$ inclusive cross section for the process $p\\stackrel{\\ensuremath{\\rightarrow}}{p}t\\overline{t}h$ in the standard model, at $\\sqrt{{s}_{H}}=14\\mathrm{TeV}.$ The next-to-leading order corrections drastically reduce the renormalization and factorization scale dependence of the Born cross section and increase the total cross section for renormalization and factorization scales larger than ${m}_{t}.$ These corrections have important implications for models of new physics involving the top quark.","journal":"Physical Review D","year":2003,"id":9304,"datarank":0.7379971388742189,"base_score":4.919980925828125,"endowment":4.919980925828125,"self_citation_contribution":0.7379971388742189,"citation_network_contribution":0.0,"self_endowment_contribution":0.7379971388742189,"citer_contribution":0.0,"corpus_percentile":null,"corpus_rank":null,"citation_count":136,"citer_count":0,"citers_with_citation_signal":0,"citers_with_endowment":0,"datacite_reuse_total":0,"is_dataset":false,"is_dataset_confidence":0.0582,"is_oa":false,"file_count":0,"downloads":0,"has_version_chain":false,"published_date":"2003-04-17","fair_score":null,"fair_percentile":null,"algorithm_id":"datarank_citation_only_1hop_v6","ranking_scope":"data_only","authors":[{"id":2262,"name":"L. H. Orr","orcid":null,"position":1,"is_corresponding":false},{"id":2263,"name":"L. Reina","orcid":null,"position":2,"is_corresponding":false},{"id":2264,"name":"D. Wackeroth","orcid":null,"position":3,"is_corresponding":false},{"id":2260,"name":"S. Dawson","orcid":"0000-0002-5598-695X","position":0,"is_corresponding":true}],"reference_count":15,"raw_metadata":null,"created_at":"2026-03-01T18:20:47.508186Z","pmid":null,"pmcid":null,"fwci":null,"citation_percentile":null,"influential_citations":0,"oa_status":null,"license":null,"views":0,"total_file_size_bytes":0,"version_count":0,"fair_f":null,"fair_a":null,"fair_i":null,"fair_r":null,"fair_zscore":null,"fair_rationale":null,"fair_model":null,"fair_agent_version":null,"fair_fulltext_source":null,"fair_has_llm":null,"fair_computed_at":null,"clinical_trials":[],"software_tools":[],"db_accessions":[],"linked_datasets":[],"topics":[]}