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Titlebook: Hadron Structure and Lepton-Hadron Interactions; Cargèse 1977 Maurice Lévy,Jean-Louis Basdevant,Jean Zinn-Justin Book 1979 Plenum Press, Ne

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Georg Glaeser,Werner Nachtigallrticular attention will be paid to the recent results presented by experimental lecturers at this school 1–3). Free use will be made of the quark-parton and gauge technology developed by other theoretical lecturers 4,5). It will not often enter explicitly, but where a choice is necessary we will ass
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https://doi.org/10.1007/978-3-319-76801-4 consists of colored quarks coupled to a color octet of Yang-Mills vector bosons. This theory can be solved in the short distance region using renormalization group methods as the effective-coupling constant vanished in this limit. This “asymptotic freedon” at short distance provides a fundamental b
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Women’s Studies: A View from the Marginss (QCD). There are many excellent reasons for believing in this theory. It embodies the broken symmetries, SU(3) and chiral SU(3)×SU(3), of the strong interactions and reflects the success of (albeit crude) quark models in explaining the spectrum of the observed hadrons. The hidden quantum number of
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https://doi.org/10.1007/978-3-319-91620-0f the interaction is superrenormalizable, the problem has been solved for both interacting bosons. and fermions.: of course technical details may change from theory to theory. When the interaction is renormalizable new difficulties arise.; they are not completely understood at the present moment.
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https://doi.org/10.1007/3-7908-1656-6pionization graphs (tower plus non- planar) in some relevant Lagrangian field theory. Since so much material has already been presented concerning non-Abelian physics at this Summer Institute, and partly to remind us that much high- energy phenomenology is still couched in the language of non-non- A
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The Roots of Communitarian Ideas,e most natural extensions of the Weinberg-Salam model in order to accomodate the recent atomic Bismuth experimental results. The differences between the model predictions in neutrino reactions are small except for the elastic υμe and υμe cross sections. We remark on the other specific experiments wh
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