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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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11#
發(fā)表于 2025-3-23 12:29:21 | 只看該作者
The European Union after Lisbonect up to 15 fbˉ. 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 j
12#
發(fā)表于 2025-3-23 13:55:07 | 只看該作者
13#
發(fā)表于 2025-3-23 18:07:10 | 只看該作者
Hadron Colliders, the Standard Model, and Beyondr quantum field theory, based on the set of fields displayed in Table 1, and the gauge symmetries .(3) x .(2) x .(1).. There are three generations of quarks and leptons, labeled by the index i = 1,2,3, and one Higgs field, ..
14#
發(fā)表于 2025-3-23 23:59:13 | 只看該作者
Tevatron Collider Run II Status 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.
15#
發(fā)表于 2025-3-24 05:32:18 | 只看該作者
16#
發(fā)表于 2025-3-24 06:35:41 | 只看該作者
17#
發(fā)表于 2025-3-24 11:12:36 | 只看該作者
18#
發(fā)表于 2025-3-24 14:56:48 | 只看該作者
Saturation Effects in Hadronic Cross Sectionsting observations at the HERA experiments [1]. The experimental results show a rise of the total γ*. cross section,.with increasing c.m. energy √s which becomes stronger with increasing photon virtuality ...
19#
發(fā)表于 2025-3-24 20:13:31 | 只看該作者
Heavy Flavour Production at D?rks. 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 ...ˉ environment.
20#
發(fā)表于 2025-3-25 02:09:25 | 只看該作者
Heavy Quark Production at CDF. and gluon fusion, .. In . collisions, the quark crosssections are convoluted with the parton density functions, ., to obtain the hadro-production quark cross-sections as follows: . where y and . are the produced quark and anti-quark rapidities, and . is the tranverse momemtum.
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