'Gluon distribution' diaporamas de présentation

QCD results from colliders

2007 Aspen Winter Conference Wesley H. Smith U. Wisconsin - Madison January 11, 2007 Outline: Parton Density Functions & Structure Functions Jets & Measurements of ? S Multijets, Inclusive Jets, W + Jets, Dijets Prompt Photons Diffraction This talk is available on:

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HERA and the LHC Report on the workshop on HERA ?LHC

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Spin Physics with eRHIC

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QCD at High Energies at HERA

QCD at High Energies at HERA. Max Klein DESY Zeuthen ICHEP 04 Beijing 21 st of August, 2004. The Quark Structure of the Proton The Strong Coupling Constant and xg Heavy Flavour Production Diffractive ep Scattering New Ideas and Developments First Results at HERA II and Outlook. s.

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Jet Quenching: What it really measures?

Jet Quenching: What it really measures?. Xin-Nian Wang Lawrence Berkeley National Laboratory. High-pT physics at LHC, Jyvaskyla, March 21-27,2007. Jet Quenching in A+A Collisions. leading particle. hadrons. q. q. hadrons. leading particle. Leading particle suppressed. hadrons. q. q.

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Antishadowing effect in the unitarized BFKL equation

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Probing the Dense Medium in Cold Nuclei -- Gluon Saturation at small-x

Probing the Dense Medium in Cold Nuclei -- Gluon Saturation at small-x. Bowen Xiao (CCNU) Feng Yuan (LBNL). Gluon saturation inevitable at small-x. QCD evolution drives the gluon distribution rising at small-x. BFKL evolution becomes relevant at small-x.

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Stato di ZEUS

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International Workshop on Transverse Polarisation Phenomena in Hard Processes

International Workshop on Transverse Polarisation Phenomena in Hard Processes Como, September 7- 10, 2005. SINGLE AND DOUBLE SPIN INTERACTIONS AT GSI. Marco Maggiora Dipartimento di Fisica ``A. Avogadro'' and INFN - Torino, Italy. Introduction. SIS300 @ GSI:

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Resummation in High Energy Scattering -- BFKL vs Sudakov

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STAR azimuthal correlations of forward di-pions in d+Au collisions in the Color Glass Condensate

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?-measurements

?-measurements. Saskia Mioduszewski. Martin Codrington. Texas A&M Group Ahmed M. Hamed. BNL 10-17-07. ?-measurements. ?+nucleus e - +e + +nucleus. e+nucleus e - +?+nucleus.

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New perspective of QCD at high energy - introduction to Color Glass Condensate -

New perspective of QCD at high energy - introduction to Color Glass Condensate -. Kazunori Itakura Service de Physique Theorique CEA/Saclay, France. Plan of the lectures. I. 1. Introduction and overview 2. Kinematics and Evolution equations

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Soft gluon resummation in transversely polarized Drell-Yan process at small transverse momentum

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F 2 bb from muon+jet final states at Z EUS

F 2 bb from muon+jet final states at Z EUS. B. Kahle, DESY Hamburg. Introduction Beauty measurements Beauty contribution to F 2 Summary and Conclusions. Motivation.

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TMDs in nuclei

TMDs in nuclei. Jian Zhou Temple University. Based on paper: Phys.Rev.D77:125010,2008. e-Print: arXiv:0801.0434 [hep-ph] by Liang, Wang and JZ. Outline:. Brief review on k T broadening phenomena Nuclear TMDs and k T broadening

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Inclusive Jet Cross Section Jet Energy Corrections

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Physics Potential of an ep Collider at the VLHC

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BFKL equation at finite temperature

BFKL equation at finite temperature. Kazuaki Ohnishi (Yonsei Univ.) In collaboration with Su Houng Lee (Yonsei Univ.). arXiv:0707.1451 [hep-ph]. Introduction Color Glass Condensate at zero T BFKL Eq. at finite T Summary. 1. Introduction. Relativistic Heavy Ion Collision experiments.

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?G from ?0 A LL

?G from ?0 A LL. A.Bazilevsky RHIC Spin Collaboration meeting November 9, 2006. ?0 A LL : ?G constrain. Fractional contribution to pp ?? 0 X at ?s=200 GeV at ? ~0. ? 0 production is sensitive to gluon distribution. PHENIX Preliminary Run5 pi0 A LL. 40% scale uncertainty is not included.

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