Understanding forward particle production Opportunities for Drell-Yan Physics at RHIC May 13 th, 2011 Roman Pasechnik Uppsala University, THEP group 1.

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Presentation transcript:

Understanding forward particle production Opportunities for Drell-Yan Physics at RHIC May 13 th, 2011 Roman Pasechnik Uppsala University, THEP group 1 In collaboration with B. Kopeliovich (USM, Chile)

We will talk about...  Color neutralization and soft physics in diffractive DIS  Sudakov suppression and elastic scattering  Drell-Yan at high energies: diffractive vs inclusive  Large and small dipoles  Eikonalization of the elastic amplitude and gap survival  Summary 2

z time Perturbative color neutralization Soft/semihard color neutralization Lack of absorptive effects!  Both include unitarity corrections and color neutralisation  Both diffractive – nondiffractive processes ? Color screening effects in different asymptotics 3

Color screening in diffractive DIS Hard part conventional (small distance) Soft part: color-screening (octet) multigluon exchange (large distance) Diffractive DIS at HERA QCD rescattering model Pasechnik, Enberg, Ingelman, Phys.Rev. D82 (2010)

5 Sudakov suppression and elastic scattering Color neutralization is automatic, no radiation into the gap, small M X is produced, no need in Sudakov! Color neutralization is required for diffraction Hard gluon Bremsstrahlung contributes at larger M X soft gluons – a part of UGDF! X For diffractive small M X production Sudakov suppression is needed!

Photon radiation in the forward quark scattering …in inelastic collision …in elastic collision Radiation depends on the whole strength of the kick rather on its structure No radiation from a quark at Pt=0! 6

Diffractive Drell-Yan in the dipole-target scattering By optical theorem Amplitude of DDY in the dipole-target scattering dipoles with different sizes interact differently! 7

Diffractive Drell-Yan in pp scattering: amplitude B. Kopeliovich, I. Potashnikova, I. Schmidt and A. Tarasov, Phys. Rev. D74, (2006) Diffractive DY amplitude..probing large distances in the proton 8

QCD factorization breaking in diffractive Drell-Yan Diffractive DY amplitude Golec-Biernat-Wuestoff (GBW) dipole cross section Interplay between hard and soft scales Difference between two Fock states Diffractive DIS Diffractive DY Dramatic breakdown of the QCD factorization! The QCD factorization holds!

Small and large dipoles 9 Golec-Biernat-Wuestoff (GBW) parameterization Kopeliovich- Schafer -Tarasov (KST) parameterization Fitted to DIS data Fitted to soft data DDY! Phys. Rev. D 62 (2000),

Eikonalization of the diffractive Drell-Yan amplitude 9 Accounts for soft and hard components on the same footing! DDY eikonalized amplitude

Diffractive Drell-Yan in pp scattering: cross section In the forward limit Proton wave function Valence quark distribution + antiquarks!

Gap survival vs. eikonalization Regge parameterization for F2 Cudell, Soyez, Phys.Lett. B516 (2001), 77

Gap survival vs. eikonalization

Diffractive vs. inclusive DY

Theory uncertainties

Conclusions  A quark cannot radiate photon diffractively in the forward direction  A hadron can radiate photon diffractively in the forward direction because of the transverse motion of quarks  The ratio diffractive/inclusive DY cross sections falls with energy and rises with photon dilepton mass due to the saturated shape of the dipole cross section  Hard and soft interactions contribute to the DDY on the same footing, which is the dramatic breakdown of the QCD factorisation  Main features of Drell-Yan diffraction are valid for other Abelian processes  Experimental measurements of DDY would allow to probe directly the dipole cross section at large separations, as well as the proton structure function at soft and semihard scales, and large x  DDY is a good playground for diffractive production of heavy flavors