Hadron production in the forward rapidity region is considered in the Color Glass Condensate approach to high energy deuteron-nucleus collisions. The projectile deuteron is treated via collinear factorization and pQCD formalism while the nucleus is described as a Color Glass Condensate. It is shown
The color glass condensate and hadron production in the forward region
β Scribed by Adrian Dumitru; Arata Hayashigaki; Jamal Jalilian-Marian
- Publisher
- Elsevier Science
- Year
- 2006
- Tongue
- English
- Weight
- 859 KB
- Volume
- 765
- Category
- Article
- ISSN
- 0375-9474
No coin nor oath required. For personal study only.
β¦ Synopsis
We consider one loop corrections to single inclusive particle production in parton-nucleus scattering at high energies, treating the target nucleus as a color glass condensate. We prove by explicit computation that in the leading log Q 2 approximation, these corrections lead to collinear factorization and DGLAP evolution of the projectile parton distribution and hadron fragmentation functions. In single-inclusive cross sections, only two-point functions of Wilson lines in the adjoint and fundamental representations (Mueller's dipoles) arise, which can be obtained from the solution of the JIMWLK equations. The application of our results to forward-rapidity production shows that, in general, recoil effects are large. Hence, the forward rapidity region at RHIC is rather different from the central region at LHC, despite comparable gluon densities in the target. We show that both the quantum x-evolution of the high-density target as well as the DGLAP Q 2 -evolution of the parton distribution and fragmentation functions are clearly seen in the BRAHMS data. This provides additional strong evidence for the color glass condensate at RHIC.
π SIMILAR VOLUMES
In this talk, we discuss some general properties of particle production in a field theory coupled to strong time dependent sources, and techniques to compute the spectrum of the produced particles in such theories. We also discuss the application of these results to the description of hadron or heav