Workshop on Grand Unification, Volume 6, Part 1985 |
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Page 143
This is the question of why the energy scale of weak interaction symmetry
breaking is so much smaller than that of unification. The problem arises because
eigenvalues of Higgs boson fields are continuously variable parameters, which ...
This is the question of why the energy scale of weak interaction symmetry
breaking is so much smaller than that of unification. The problem arises because
eigenvalues of Higgs boson fields are continuously variable parameters, which ...
Page 144
Symmetry breaking by Wilson lines is unusual as a topological approach to
grand unified symmetry breaking that does not have harmful implications for the
fermion quantum numbers. Now we turn to a discussion of gauge and Yukawa ...
Symmetry breaking by Wilson lines is unusual as a topological approach to
grand unified symmetry breaking that does not have harmful implications for the
fermion quantum numbers. Now we turn to a discussion of gauge and Yukawa ...
Page 394
Non-gravitational radiative corrections may then determine not only the scale of
22) ~ weak gauge symmetry breaking (of order |1q(11)) but also the scale m ~ 43
) of global supersymmetry breaking m ~ m. . - 0(Mn ) , of local super- ' 44) ...
Non-gravitational radiative corrections may then determine not only the scale of
22) ~ weak gauge symmetry breaking (of order |1q(11)) but also the scale m ~ 43
) of global supersymmetry breaking m ~ m. . - 0(Mn ) , of local super- ' 44) ...
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Bibliographic information
| Title | Workshop on Grand Unification, Volume 6, Part 1985 Volume 11 of Lie groups Progress in physics |
| Authors | Serge Rudaz, Thomas F. Walsh |
| Publisher | Math Sci Press |
| Original from | Cornell University |
| Digitized | Apr 11, 2011 |
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