Titlebook: New Aspects of High-Energy Proton-Proton Collisions; Ahmed Ali Book 1988 Springer Science+Business Media New York 1988 Boson.CERN.Cross se

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gentle

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Higgs Production in High Energy Hadron Collisions,edients and loose ends which can only be answered if new facilities will come into operation. In particular, the top quark and the Higgs boson have to be yet discovered. The experimental determination of the values of their masses will provide fundamental information on the validity of the Higgs mec

防銹

Cosmopolitan

Signatures of Compositeness in Very High Energy pp Collisions,tely, the energy range addressed at this meeting on future pp collisions is comfortably high, ranging from √s = 17 TeV at the LHC at CERN over 20 to possibly 40 TeV at SSC to 100 TeV at the further reaching ELOISATRON project. So, I can afford to focus on scenarios of compositeness which are disting

輕率的你

Physics of Superheavy Onia,er-high-energy proton-proton colliders. Various aspects of superheavy onia go beyond the na?ve extrapolation from known light and heavy onium systems. The empirical “constant” law for the leptonic width no longer holds; The pseudoscalar is the predominantly produced state in . collisions.

cinder

Beauty Physics at the Ultrahigh Energies of the ELOISATRON, Synchrotron) is compared with possibilities at 40 TeV at the Superconducting Super Collider. The effect of the increase in center of mass energy on the production and decay of B mesons has been investigated, particularly with respect to the accumulation of large samples of B hadron decays necessary

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Enervate

Prompt Photons in Very High Energy Collisions,ng our knowledge of the proton [1,2,3,4]. The fact that the photon has a pointlike interaction with the quark makes it, indeed, a good probe of hadrons and allows precise QCD predictions. It turns out that, at present energies --13 GeV ≤ √S ≤ 630 GeV--, the agreement between data and theory is spect

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