Entrancing 发表于 2025-3-23 12:29:21
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 jClassify 发表于 2025-3-23 13:55:07
http://reply.papertrans.cn/43/4205/420419/420419_12.pngfibroblast 发表于 2025-3-23 18:07:10
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, ..Alveoli 发表于 2025-3-23 23:59:13
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.Yag-Capsulotomy 发表于 2025-3-24 05:32:18
http://reply.papertrans.cn/43/4205/420419/420419_15.pngCoronary-Spasm 发表于 2025-3-24 06:35:41
http://reply.papertrans.cn/43/4205/420419/420419_16.pngAncillary 发表于 2025-3-24 11:12:36
http://reply.papertrans.cn/43/4205/420419/420419_17.png敌意 发表于 2025-3-24 14:56:48
Saturation Effects in Hadronic Cross Sectionsting observations at the HERA experiments . 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 ...反复拉紧 发表于 2025-3-24 20:13:31
Heavy Flavour Production at DØrks. 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.割公牛膨胀 发表于 2025-3-25 02:09:25
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.