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Volumn 59, Issue 11, 1999, Pages

Embedding phenomenological quark-lepton mass matrices into SU(5) gauge models

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Indexed keywords


EID: 85037914579     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.59.113016     Document Type: Article
Times cited : (41)

References (34)
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    • Cambridge University Press, Cambridge, England
    • J.N. Bahcall, Neutrino Astrophysics (Cambridge University Press, Cambridge, England, 1989);
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    • Bahcall, J.N.1
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    • Super-Kamiokande Collaboration, Y. Fukuda, Phys. Rev. Lett. 81, 1562 (1998).
    • (1998) Phys. Rev. Lett. , vol.81 , pp. 1562
    • Fukuda, Y.1
  • 25
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    • Fukugita, Tanimoto, and Yanagida
    • Fukugita, Tanimoto, and Yanagida 7.
  • 26
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    • Harari, Haut, and Weyers
    • Harari, Haut, and Weyers 6.
  • 27
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    • See S. Pakvasa and H. Sugawara, Phys. Lett. 73B, 61 (1978), as an early attempt to construct a gauge theory compatible with discrete symmetry. This model was not successful in giving empirically acceptable mass-mixing relations.
    • (1978) Phys. Lett. , vol.73B , pp. 61
    • Pakvasa, S.1    Sugawara, H.2
  • 28
    • 85037893625 scopus 로고    scopus 로고
    • Koide
    • Koide 6 (1989).
  • 29
    • 85037898021 scopus 로고    scopus 로고
    • Let us assume that heavy (Formula presented) transform as (Formula presented) under (Formula presented) Then the Yukawa coupling (Formula presented) may be taken as (Formula presented) We may also assume that the Majorana mass matrix (Formula presented) takes an (Formula presented)-invariant form (Formula presented) Integration of (Formula presented) then gives (Formula presented) If (Formula presented) is given by (Formula presented) we have (Formula presented) for the SUSY unification scale (Formula presented); in this case we expect (Formula presented).
    • Let us assume that heavy (Formula presented) transform as (Formula presented) under (Formula presented) Then the Yukawa coupling (Formula presented) may be taken as (Formula presented) We may also assume that the Majorana mass matrix (Formula presented) takes an (Formula presented)-invariant form (Formula presented) Integration of (Formula presented) then gives (Formula presented) If (Formula presented) is given by (Formula presented) we have (Formula presented) for the SUSY unification scale (Formula presented); in this case we expect (Formula presented).
  • 30
    • 85037882278 scopus 로고    scopus 로고
    • Our matrix elements are assumed to be all real for simplicity of the model. It is possible to introduce phases. In fact, there is a well-known mismatch between down quark masses and the Cabibbo angle with natural relation (14): if experimental values are put into the right-hand side of Eq. (14), (Formula presented) somewhat deviates from experiment, and this problem is usually cured by introducing phases (see Fritzsch
    • Our matrix elements are assumed to be all real for simplicity of the model. It is possible to introduce phases. In fact, there is a well-known mismatch between down quark masses and the Cabibbo angle with natural relation (14): if experimental values are put into the right-hand side of Eq. (14), (Formula presented) somewhat deviates from experiment, and this problem is usually cured by introducing phases (see Fritzsch 5). Our model also inherits this problem. If we introduce phases for all matrix elements, we can give the right value for (Formula presented) and also fit (Formula presented) (Formula presented) changes very little and (Formula presented) can be larger than our prediction (discussed below) by up to 50% (hence the real phase is favored for (Formula presented). In this paper we do not dare to pursue precise agreement with experiment, keeping the simplicity of the model, since the introduction of phases modifies the model only at a quantitative level.
  • 32
    • 85037896067 scopus 로고    scopus 로고
    • It is unclear whether perturbative analysis applies to a very light quark mass, especially to (Formula presented) and (Formula presented) Here we take them to guide our considerations.
    • It is unclear whether perturbative analysis applies to a very light quark mass, especially to (Formula presented) and (Formula presented) Here we take them to guide our considerations.


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