-
7
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-
84931541544
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-
At higher order there are dependences on the spectrum of the theory; however, it is remarkable how insensitive sinsup 2 theta W is to the details of this spectrum.
-
-
-
-
12
-
-
84931541545
-
-
Arason et al., Ref. 14
-
-
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-
14
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-
84931541546
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-
Kelley, Lopez, and Nanopoulos, Ref. 14
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-
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35
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84931541481
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-
Q. Shafi and B. Ananthanarayan, in 1991 Summer School in High Energy Physics and Cosmology, Proceedings of the Trieste Summer School, Trieste, Italy, edited by E. Gava et al. (World Scientific, Singapore, 1992), p. 233.
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-
-
-
39
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-
84931541480
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-
A prediction can be made for the ratio mt / sin β in SU(5), but not directly on the top quark mass.
-
-
-
-
40
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-
84931541479
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-
Such a prediction can also be made in nonsupersymmetric SO(10) theories. However, whatever mechanism is used to rectify the sinsup 2 theta W prediction in the theory will also affect the top prediction, making it much more model dependent.
-
-
-
-
42
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-
84931541477
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-
in Proceedings of the Second IFT Workshop on Yukawa Couplings and the Origins of Mass, 1994 (unpublished);
-
-
-
-
56
-
-
84931541476
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-
see also the appendix in Barger, Berger, and Ohmann, Ref. 14
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-
-
-
61
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84931541475
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-
edited by, R. Orava, P. Eerola, M. Nordberg, World Scientific, Singapore, Vol. I, p. 309, and references therein.
-
(1992)
Physics and Experiments with Linear Colliders, Proceedings of the Workshop, Saariselkä, Finland, 1991
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-
Zwirner, F.1
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63
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84931541493
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-
Particle Data Group, K. Hikasa et al., Phys. Rev. D 45,S1 (1992).
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-
-
-
70
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-
4243999689
-
-
If for some reasons GUT and Planck scale corrections to the gauge couplings are known, then α3 ( mZ ) becomes a function of the superpartner spectrum and, in particular, of the Higgsino mass. The dependence may be found in
-
(1992)
Phys. Rev. Lett.
, vol.69
, pp. 1014
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-
Hisano, J.1
Murayama, H.2
Yanagida, T.3
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72
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84931541495
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-
Giveon, Hall, and Sarid, Ref. 31
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-
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73
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84931541489
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-
and Langacker and Polonsky, Ref. 20
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-
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75
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84931541490
-
-
Langacker and Polonsky, Ref. 20
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-
-
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77
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84931541457
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-
The approximate equality of the coefficients of yG in the RGE of λt,b,τ becomes an exact one when the right handed neutrino is included in the low energy theory. This is a consequence of the Pati Salam subgroup G PS equivSU(2)sub L ×SU(2)sub R timesSU(4) of SO(10), which is only broken in the Yukawa sector by the removal of νR. In practice, GPS is manifested when yG > αG, in which case the three Yukawa couplings run almost in parallel.
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