Abstract

We discuss emergence of geometrical scaling as a consequence of the nonlinear evolution equations of QCD, which generate a new dynamical scale, known as the saturation momentum: Qs. In the kinematical region where no other energy scales exist, particle spectra exhibit geometrical scaling (GS), i.e. they depend on the ratio pT=Qs, and the energy dependence enters solely through the energy dependence of the saturation momentum. We confront the hypothesis of GS in different systems with experimental data.

Highlights

  • In this report we present a concise analysis of geometrical scaling (GS), slightly extended with respect to the presentation given at the XLVI International Symposium on Multiparticle Dynamics

  • Case, in the right panel where we plot R for λ = 0.32 no GS is seen. In this short note we have argued that geometrical scaling is clearly seen in the Deep inelastic scattering (DIS) and pp data

  • Phenomenological analysis analogical to the one described here has been used to look for the effects of GS in pA and heavy ion collisions and in pT correlation with multiplicity [2]–[5]

Read more

Summary

Introduction

In this report we present a concise analysis of GS, slightly extended with respect to the presentation given at the XLVI International Symposium on Multiparticle Dynamics. In QCD we have basically two sets of evolution equations that describe the change of parton densities with decreasing resolution scale 1/Q2 – DGLAP equations, or with growing energy (or equivalently with decreasing Bjorken x) – BFKL equation. In both cases the number of partons, or more precisely the number of gluons, is growing rapidly with the evolution variable. The travelling wave corresponds to the scaling solution with the saturation momentum given by Eq (1).

Inelastic pT spectra at the LHC
Electron-positron scattering
Summary

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.