Fluctuations, Saturation, and Diffractive Excitation in High Energy Collisions
arXiv:1004.5502 · doi:10.1007/JHEP10(2010)014
Abstract
Diffractive excitation is usually described by the Good--Walker formalism for low masses, and by the triple-Regge formalism for high masses. In the Good--Walker formalism the cross section is determined by the fluctuations in the interaction. In this paper we show that by taking the fluctuations in the BFKL ladder into account, it is possible to describe both low and high mass excitation by the Good--Walker mechanism. In high energy collisions the fluctuations are strongly suppressed by saturation, which implies that pomeron exchange does not factorise between DIS and collisions. The Dipole Cascade Model reproduces the expected triple-Regge form for the bare pomeron, and the triple-pomeron coupling is estimated.
20 pages, 12 figures
References in corpus (6)
- A QCD motivated model for soft interactions at high energies
- Soft processes at the LHC, I: Multi-component model
- Soft processes at the LHC, II: Soft-hard factorization breaking and gap survival
- Elastic and quasi-elastic and scattering in the Dipole Model
- Description of soft diffraction in the framework of reggeon calculus. Predictions for LHC
- On the High Energy Behaviour of The Total Cross Section in the QCD Dipole Model
Cited by in corpus (9)
- Diffractive and non-diffractive wounded nucleons and final states in pA collisions
- A comprehensive model of soft interactions in the LHC era
- Forward-Central Jet Correlations at the Large Hadron Collider
- Correlations in double parton distributions at small x
- Light hadron production in inclusive pp-scattering at LHC
- Diffractive excitation in and collisions at high energies
- Total, inelastic and (quasi-)elastic cross sections of high energy pA and gamma-A reactions with the dipole formalism
- Parton Cascades, Small x, and Saturation in High Energy Collisions
- Multiparticle Dynamics in the LHC Era