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Status of the Standard Model of Particle Phenomenology
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Status of the Standard Model
Paul H. Frampton
University of North Carolina at Chapel Hill
October 2003
1 Introduction
The standard model is healthy is all respects except for the non-zero neutrino
masses which require an extension of the minimal version.
This talk was in three parts:
(I) Rise and Fall of the Zee Model 1998-2001.
(II) Classification of Two-Zero Textures.
(III) FGY Model relating Cosmological B to Neutrino CP violation.
For parts (I) and (II) references are provided. Part (III) is included in
this write-up.
2 Rise and Fall of the Zee Model 1998-2001
This first part was based on:
P.H. Frampton and S.L. Glashow, Phys. Lett. 461, 95 (1999). hep-ph/9906375.
3 Classification of Two-Zero Textures
The second part was based on:
P.H. Frampton, S.L. Glashow and D. Marfatia, Phys. Lett. B536, 79
(2002). hep-ph/0201008
4 FGY Model relating Cosmological B with Neu-
trino CP Violation
One of the most profound ideas is[1] that baryon number asymmetry arises
in the early universe because of processes which violate CP symmetry and
1
that terrestrial experiments on CP violation could therefore inform us of the
details of such cosmological baryogenesis.
The early discussions of baryogenesis focused on the violation of baryon
number and its possible relation to proton decay. In the light of present
evidence for neutrino masses and oscillations it is more fruitful to associate
the baryon number of the universe with violation of lepton number[2]. In
the present Letter we shall show how, in one class of models, the sign of the
baryon number of the universe correlates with the results of CP violation in
neutrino oscillation experiments which will be performed in the forseeable
future.
Present data on atmospheric and solar neutrinos suggest that there are
respective squared mass differences ?a ? 3×10?3eV 2 and ?s ? 5×10?5eV 2.
The corresponding mixing angles θ1 and θ3 satisfy tan
2θ1 ? 1 and 0.6 ≤
sin22θ3 ≤ 0.
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