Scholarlink

Abstract <p>New evidence for the dominance of the Balitsky–Fadin–Kuraev–Lipatov (BFKL) evolution effects is obtained by comparison of the calculation of Meueller–Navelet (MN) dijet production cross section in the next-to-leading logarithmic approximation of the BFKL evolution with the recent CMS measurement at the LHC at 2.76 TeV. Here the MN dijet is the maximally separated in rapidity pair of jets with both jets taken among jets with transverse momentum above some chosen <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11497_2025_10036_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="42" /> </InlineMediaObject> <EquationSource Format="TEX">\({{p}_{{ \bot \min }}}\)</EquationSource> <!--PhysPNLt2470214Egorov-m1--> </InlineEquation> in an event. Unlike the large-angle scattering Gribov–Lipatov–Altarelli–Parisi–Dokshitzer (GLAPD) evolution, the small-angle scattering BFKL evolution for is the dominant high-energy asymptotic regime of QCD.</p>

错误：搜索内容不能为空，请输入英文关键词
错误：关键词超出字数限制，请精简
高级检索

Manifestation of Asymptotic QCD Effects in Dijet Production at Large Hadron Collider with 2.76 TeV

  • 期刊论文

  • 发表日期：

    2025年2月1日

查看全文
  • A. Yu. Egorov,
  • V. T. Kim

摘要

Abstract

New evidence for the dominance of the Balitsky–Fadin–Kuraev–Lipatov (BFKL) evolution effects is obtained by comparison of the calculation of Meueller–Navelet (MN) dijet production cross section in the next-to-leading logarithmic approximation of the BFKL evolution with the recent CMS measurement at the LHC at 2.76 TeV. Here the MN dijet is the maximally separated in rapidity pair of jets with both jets taken among jets with transverse momentum above some chosen \({{p}_{{ \bot \min }}}\) in an event. Unlike the large-angle scattering Gribov–Lipatov–Altarelli–Parisi–Dokshitzer (GLAPD) evolution, the small-angle scattering BFKL evolution for is the dominant high-energy asymptotic regime of QCD.