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Titlebook: Hadron Collider Physics 2002; Proceedings of the 1 Martin Erdmann,Thomas Müller Conference proceedings 2003 Springer-Verlag Berlin Heidelbe

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D. P. Hanson,C. Lackman,T. PetinauxIn the past decade, QCD has become a quantitative science and comparisons of experimental data with NLO QCD have become the standard. However, there are many reasons why extending perturbative calculations to NNLO is vital in reducing the theoretical uncertainty. In the following we list six of them.
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https://doi.org/10.1007/978-1-4039-2000-3 has been steadily improving, but the pace has been slower than anticipated. The peak luminosity now exceeds that of Run I and sources of additional improvement to reach design goals have been identified and are being addressed. This paper summarizes the progress to date.
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Search and Seizure Measures and Their Review i.e. . ≤ 10¯.. Here and in the following, . denotes the fraction of the proton’s momentum carried by the quark that interacts with the electron. At low ., the struck quark usually results from a long cascade of parton branchings as illustrated in Fig. 1. Partons at the bottom of the cascade can carry a fraction
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Kees van Kersbergen,Barbara Visrks. Unlike the . which operate at the γ(4s) resonance, all kinds of .-hadrons . are produced. However the backgrounds at a hadron collider are considerably larger than in the relatively clean ...¯ environment.
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The European Union after Lisbonect up to 15 fb¯. of data in this new run period. The increase in instantaneous luminosity, center-of-mass energy (from 1.8 TeV to 2 TeV) and the improved acceptance of the detectors will allow stringent tests of the Standard Model (SM) predictions in extended regions of jet transverse energy, and jet pseudorapidity, η..
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