The colour octet representation of the non-forward BFKL Green function
arXiv:1112.4162 · doi:10.1016/j.physletb.2012.02.036
Abstract
We factorize the infrared divergences of the non-forward BFKL Green function for a general t-channel projection of the color quantum numbers and study the properties of the infrared finite remainder in the case of color octet exchange. The octet Green function is compared with the singlet case for different values of the momentum transfer. The octet Green function plays an important role in the calculation of the finite remainder of the two-loop six-point MHV planar amplitude in N = 4 SYM as it was demonstrated by Bartels, Lipatov and one of us in http://arXiv.org/abs/arXiv:0802.2065 and http://arXiv.org/abs/arXiv:0807.0894. A comparison with regularizations preserving conformal invariance at large momentum transfer is shown.
12 pages, 7 figures
References in corpus (14)
- Classical Polylogarithms for Amplitudes and Wilson Loops
- Hexagon Wilson loop = six-gluon MHV amplitude
- The Two-Loop Six-Gluon MHV Amplitude in Maximally Supersymmetric Yang-Mills Theory
- Bootstrapping the three-loop hexagon
- BFKL Pomeron, Reggeized gluons and Bern-Dixon-Smirnov amplitudes
- The azimuthal decorrelation of jets widely separated in rapidity as a test of the BFKL kernel
- BFKL equation for the adjoint representation of the gauge group in the next-to-leading approximation at N=4 SUSY
- NLO jet vertex from Lipatov's QCD effective action
- The effect of NLO conformal spins in azimuthal angle decorrelation of jet pairs
- Integrability of scattering amplitudes in N=4 SUSY
- BFKL approach and six-particle MHV amplitude in N=4 super Yang-Mills
- Azimuthal decorrelation of forward jets in Deep Inelastic Scattering
- High-Energy Dijets in N=4 SYM
- Collinear and Regge behavior of 2 -> 4 MHV amplitude in N = 4 super Yang-Mills theory
Cited by in corpus (30)
- Scale choice & collinear contributions to Mueller-Navelet jets at LHC energies
- Multi-Regge kinematics and azimuthal angle observables for inclusive four-jet production
- Inclusive Four-jet Production at 7 and 13 TeV: Azimuthal Profile in Multi-Regge Kinematics
- BFKL Azimuthal Imprints in Inclusive Three-jet Production at 7 and 13 TeV
- Hunting BFKL in semi-hard reactions at the LHC
- Stability of Azimuthal-angle Observables under Higher Order Corrections in Inclusive Three-jet Production
- Quark contribution to the gluon Regge trajectory at NLO from the high energy effective action
- Single bottom quark production in kT-factorisation
- The NLO N =4 SUSY BFKL Green function in the adjoint representation
- A study of the diffusion pattern in N=4 SYM at high energies
- The Dynamics of Particle-Particle Correlations and the Ridge Effect in Proton-Proton Collisions
- A Monte Carlo study of double logarithms in the small x region
- Bootstrap and momentum transfer dependence in small x evolution equations
- The next-to-leading order vertex for a forward jet plus a rapidity gap at high energies
- Inclusive three- and four-jet production in multi-Regge kinematics at the LHC
- Probing the BFKL dynamics in inclusive three jet production at the LHC
- The high-energy radiation pattern from BFKLex with double-log collinear contributions
- Solution of the Bartels-Kwiecinski-Praszalowicz equation via Monte Carlo integration
- BFKL phenomenology: resummation of high-energy logs in semi-hard processes at LHC
- Multiperipheral final states in crowded twin-jet events at the LHC
- High-energy resummation in semi-hard processes at the LHC
- Open Spin Chains and Complexity in the High Energy Limit
- Inclusive four-jet production: a study of Multi-Regge kinematics and BFKL observables
- Monte Carlo techniques in small-x physics: Formal studies and phenomenology
- The Forward Physics Facility at the High-Luminosity LHC
- Inclusive three jet production at the LHC at 7 and 13 TeV collision energies
- The High Energy Radiation Pattern from BFKLex
- Inclusive three jet production at the LHC as a new BFKL probe
- Average minijet rapidity ratios in Mueller-Navelet jets
- On the conformal spin dependence of the perturbative QCD vacuum singularity