On the conformal spin dependence of the perturbative QCD vacuum singularity
arXiv:2203.12418 · doi:10.1007/JHEP07(2022)109
Abstract
We study the four-gluon scattering amplitude in the high energy limit of QCD written in terms of its conformal expansion. We highlight the need to include both even and odd conformal spin contributions in order to map it to an iterative representation in rapidity and transverse momentum space which we have evaluated numerically. By Fourier expanding in a set of three azimuthal angles, we find a new form for the amplitude in terms of hypergeometric functions. An alternative formulation is possible when connecting this Fourier expansion with Bessel kernels studied in analytic number theory.
18 pages, 3 figures
References in corpus (13)
- The azimuthal decorrelation of jets widely separated in rapidity as a test of the BFKL kernel
- Azimuthal decorrelation of Mueller-Navelet jets at the Tevatron and the LHC
- The effect of NLO conformal spins in azimuthal angle decorrelation of jet pairs
- Jet vetoing at the LHC
- Entanglement entropy production in deep inelastic scattering
- Gaps between jets in hadronic collisions
- Azimuthal decorrelation of forward jets in Deep Inelastic Scattering
- The next-to-leading order vertex for a forward jet plus a rapidity gap at high energies
- 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 Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
- Solution of the Bartels-Kwiecinski-Praszalowicz equation via Monte Carlo integration
- Bethe Ansatz for XXX chain with negative spin