1,393 research outputs found

    Aspects of Neutrino Mass Matrices

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    After an Introduction briefly describing the rise and fall of the three-zero texture of the Zee model, we discuss still-allowed two-zero textures for the Majorana three-neutrino mass matrix. Finally, a model with two right-handed neutrinos and two Dirac texture zeros is described (FGY model) which can relate CP violation in leptogenesis to CP violation in long-baseline neutrino oscillations.Comment: 9 pages latex. Talk at Coral Gables 2003. Added reference

    Consistency Conditions for AdS/CFT Embeddings

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    The group embeddings used in orbifolding the AdS/CFT correspondence to arrive at quiver gauge field theories are studied for both supersymmetric and non-supersymmetric cases. For an orbifold AdS5×S5/ΓAdS_5 \times S^5/\Gamma the conditions for embeddings of the finite group Γ\Gamma in the SU(4)∌O(6)SU(4) \sim O(6) isotropy of S5S^5 are stated in the form of consistency rules, both for Abelian and Non-Abelian Γ\Gamma.Comment: 10 pages LaTe

    Position of First Doppler Peak

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    This talk describes an analytic calculation of the position of the first accoustic peak as a function of the matter density and the cosmological constant (work with Y.J. Ng and R. Rohm), agreeing with independent numerical studies. There is also discussion of supernovae observations and how together these approaches combine to suggest non-zero cosmological constant. An alternative to a constant vacuum density - quintessence - is mentioned.Comment: 9 pages LaTeX. Talk at COSMO-98. Asilomar, Monterey, California. November 199

    Quiver Gauge Theory and Unification at About 4 TeV

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    The use of the AdS/CFT correspondence to arrive at quiver gauge field theories is dicussed, focusing on the orbifolded case without supersymmetry. An abelian orbifold with the finite group ZpZ_{p} can give rise to a G=SU(N)pG = SU(N)^p gauge group with chiral fermions and complex scalars in different bi-fundamental representations of GG. The precision measurements at the ZZ resonance suggest the values p=12p = 12 and N=3N = 3, and a unifications scale MU∌4M_U \sim 4 TeV.The robustness and predictivity of such grand unification is discussed.Comment: 16 pages LaTeX with two eps figures. Plenary talk at SCGT02, Nagoya. Dec 200

    Outcome from Spontaneous CP Violation for B Decays

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    In the aspon model solution of the strong CPCP problem, there is a gauged U(1)U(1) symmetry, spontaneously broken by the same vacuum expectation value which breaks CPCP, whose massive gauge boson provides an additional mechanism of weak CPCP violation. We calculate the CPCP asymmetries in BB decays for the aspon model and show that they are typically smaller than those predicted from the standard model. A linear relation between the CPCP asymmetries of different decay processes is obtained.Comment: REVTEX, 9 pages, IFP-486-UNC, NSF-PT-94-1, and UDHEP-01-9
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