The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order

Abstract

We complete the computation of the Mueller-Tang jet impact factor at next-to-leading order (NLO) initiated in arXiv:1406.5625 and presented in arXiv:1404.2937 by computing the real corrections associated to gluons in the initial state making use of Lipatov's effective action. NLO corrections for this effective vertex are an important ingredient for a reliable description of large rapidity gap phenomenology within the BFKL approach.

32 pages, many figures

References in corpus (9)

• Photon impact factor in the next-to-leading order
• Description of F2 and FL at small x using a collinearly-improved BFKL resummation
• Using HERA Data to Determine the Infrared Behaviour of the BFKL Amplitude
• Gaps between jets in hadronic collisions
• The next-to-leading order vertex for a forward jet plus a rapidity gap at high energies
• ${\gamma }^{\ast }{\gamma }^{\ast }$ Cross Section at NLO and Properties of the BFKL Evolution at Higher Orders
• The quark induced Mueller-Tang jet impact factor at next-to-leading order
• Gaps between jets at hadron colliders in the next-to-leading BFKL framework
• The high energy behavior of QCD: The effective action and the triple-Pomeron-vertex

Cited by in corpus (10)

• BFKL evolution and the growth with energy of exclusive J/Psi and Upsilon photo-production cross-sections
• Pursuing the Precision Study for Color Glass Condensate in Forward Hadron Productions
• Forward Higgs production within high energy factorization in the heavy quark limit at next-to-leading order accuracy
• The quark induced Mueller-Tang jet impact factor at next-to-leading order
• Hybrid kT-factorization and impact factors at NLO
• Forward Inclusive Jet Productions in pA Collisions
• Transverse Momentum Dependent Gluon Distribution within High Energy Factorization at Next-to-Leading Order
• Jets separated by a large pseudorapidity gap at the Tevatron and at the LHC
• First computation of Mueller Tang processes using the full NLL BFKL approach
• On the conformal spin dependence of the perturbative QCD vacuum singularity