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h. Eksp. Thor. Fiz. 49 (1989) 473]. [142] E. J. Weinberg, "Multivortex Solutions Of The Ginzburg-Landau Eq
yet to be found. Another issue which should be addressed is that of the representations content of the SU(212) symmetry uncovered for the superfiag Landau model [9], within the study of quantum mechanics on super manifolds. Preliminary results indicate these are new types of short representations previ
tain the spurious gauge dependence. The Coleman-Weinberg effective action l'aff and effective potential V
lid varies with 41. We find that 14„r also changes at a level comparable to its sensitivity to Mg or Ali as the gauge pa- rameter deviates from the Landau gauge (egc = 0). It is there- fore important to consider this ambiguity for model building purposes. Nevertheless, the absolute change in lid is far
tain the spurious gauge dependence. The Coleman-Weinberg effective action f eff and effective potential V
ia varies with $4e. We find that V;,,( also changes at a level comparable to its sensitivity to Ahr or Me as the gauge pa- rameter deviates from the Landau gauge (‘ = 0). It is there- fore important to consider this ambiguity for model building purposes. Nevertheless, the absolute change in Vim is far t
t at the summer school in 1960, he began to study the literature on symmetry and symmetry breaking, examin- ing the work of Nambu, Goldstone, Salam, Weinberg, and Anderson. Higgs became depressed by the seemingly hopeless task of reconciling Goldstone's theorem with the possibility of massive Yang-Mills
losely surround the negative charge, and so at a distance the physical effects of the initial negative charge are reduced. This meant, according to Landau, that the closer you get to an elec- tron, the larger its actual charge will appear. If we measure the electron charge to be some specific value at
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