Differences between Monte Carlo models for DIS at small-x and the relation to BFKL dynamics
arXiv:hep-ph/9610535 · doi:10.1016/S0370-2693(96)01637-1
Abstract
The differences between two standard Monte Carlo models, Lepto and Ariadne, for deep inelastic scattering at small-x is analysed in detail. It is shown that the difference arises from a `unorthodox' suppression factor used in Ariadne which replaces the normal ratio of parton densities. This gives rise to a factor that qualitatively is similar to what one would expect from BFKL dynamics for some observables like the energy flow and forward jets but not for the 2+1 jet cross-section. It is also discussed how one could use the 2+1 jet cross-section as a probe for BFKL dynamics.
10 pages Latex, 4 eps figures
References in corpus (13)
- Parton Distributions of the Proton
- A Measurement and QCD Analysis of the Proton Structure Function at HERA
- A Measurement of the Proton Structure Function
- Measurement of the Proton Structure Function at low and low at HERA
- Dijet Production at HERA in Next-to-Leading Order
- Transverse Energy and Forward Jet Production in the Low Regime at HERA
- Associated Jet Production at HERA
- Measurement of from Jet Rates in Deep Inelastic Scattering at HERA
- QCD Predictions for the Transverse Energy Flow in Deep-Inelastic Scattering in the Small x HERA Regime
- Dijet Production at HERA as a Probe of BFKL Dynamics
- Projet: Jet Cross Sections in Deeply Inelastic Electron Proton Scattering (VERSION 4.1)
- Renormalization scale uncertainty in tne DIS 2+1 jet cross-section
- Jet production in high Q^2 deep-inelastic eo scattering at HERA