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In our conventions, H1 is the Higgs boson coupled to charged leptons and down-type quarks, H2 the Higgs boson coupled to up-type quarks.
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14
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84927407498
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As we will see in Sec. II, in order to avoid an axion there must also be other terms in W, such as (k/3)N3.
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17
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84927407496
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Report No. CERN-TH.4931/87 (unpublished);
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18
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84927407495
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Report No. CERN-TH.5005/88 (unpublished);
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36
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84927407494
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If the pseudoscalar with mass 3kxAk is the lighter of the two pseudoscalars, then γ -> π /2, and we must interchange P1<-> P2 in the following discussion.
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37
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84927407493
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Technically, one might also require that this zero-field configuration should not be a local minimum of the potential, entailing that at least one of the soft mass-squared terms in the potential of Eq. (2.6) be negative. This condition would be imposed in order to avoid any possibility that the hot universe, originally in the symmetric vacuum, would be trapped in this metastable state at a temperature below that of the phase transition to the asymmetric vacuum. This is a somewhat model-dependent scenario, and we have not imposed such a condition on our parameters. However, we have checked that imposing this condition on the model-independent analysis of this section leads to very minor changes—the bounds on the Higgs-boson masses are slightly more restrictive in a very narrow range of parameter space when r is large. The renormalization-group analysis of Sec. V (which favors small r) is completely unaffected.
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38
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However, this has not yet been proven as a theorem.
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Since MSUSY is in general not much larger than mW, the reader might wonder why we introduce this new threshold. The reason is that, if one uses naively the supersymmetric renormalization-group equations, some of the parameters (e.g., mH2 2) have very large variations between MSUSY and mW, making such an approximation unreliable.
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49
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Note that the assumptions mU!= 0, MU=AU=0 and AU!= 0, mU=MU=0 would not correspond to phenomenologically acceptable scenarios.
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50
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S. L. Wu, in Lepton and Photon Interactions, Proceedings of the 1987 International Symposium on Lepton and Photon Interactions at High Energies, Hamburg, West Germany, 1987, edited by W. Bartel and R. Rückl
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(1987)
Nucl. Phys. B, Proc. Suppl.
, vol.3
, pp. 39
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60
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This is related to the fact that our solutions turn out to have tanβ > 1.4. For tanbeta strictly equal to 1, mS1 =0 since the determinant of the scalar mass matrix is zero in that case.
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61
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contributed paper to the 24th International Conference on High Energy Physics
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M. Narain et al.., contributed paper to the 24th International Conference on High Energy Physics, Munich, August, 1988.
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(1988)
Munich
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Narain, M.1
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63
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Convenient references for detection of a light Higgs boson at an e+e- machine are Physics at LEP, LEP Jamboree, Geneva, Switzerland, 1985, edited by J. Ellis and R. Peccei (CERN Report No. 86-02, Geneva, 1986); Proceedings of the 2nd Mark II Workshop on SLC Physics, Granlibakken, 1986, edited by K. Krieger (SLAC Report No. 306, Granlibakken, 1986).
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Studies of physics at high-energy e+e- colliders have been surveyed in C. Ahn et al.. (SLAC Report No. 329, 1988) (unpublished); Proceedings of the Workshop on Physics at Future Accelerators, La Thuile, Italy, 1987, edited by J. H. Mulvey (CERN Report No. 87-07, Geneva, Switzerland, 1987).
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0000788579
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A study of charged-Higgs-boson detection in quark decay modes appears in
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(1988)
Phys. Rev. B
, vol.38
, pp. 2158
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Komamiya, S.1
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D. Atwood, J. Brau, J. Gunion, G. Kane, R. Madaras, D. Miller, L. Price, and L. Spadafora, in Experiments, Detectors, and Experimental Areas for the Supercollider, proceedings of the Workshop, Berkeley, California, 1987, edited by R. Donaldson and M. Gilchriese (World Scientific, Singapore, 1987), p. 728.
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71
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J. F. Gunion, H. E. Haber, S. Komamiya, H. Yamamoto, and A. Barbaro-Galtieri, Experiments, Detectors, and Experimental Areas for the Supercollider, edited by R. Donaldson and M. Gilchriese (World Scientific, Singapore, 1987), p. 110.
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