Abstract
Randall-Sundrum models provide a possible explanation of (gauge-gravity) hierarchy, whereas discrete symmetry flavor groups yield a possible description of the texture of Standard Model (SM) fermion masses. We use both these ingredients to propose a five-dimensional extension of the Standard Model where the mass hierarchy of the four-dimensional effective field theory is obtained only using localization parameters of order 1. We consider a bulk custodial gauge symmetry group together with an Abelian ${Z}_{4}$ group: the model turns out to yield a rather minimal extension of the SM as it only requires two brane Higgs fields to provide the desired Yukawa interactions and the required spontaneous symmetry breaking pattern. In fact, the presence of an extra dimension allows the use of the Scherk-Schwarz mechanism to contribute to the breaking of the bulk custodial group down to the SM gauge symmetry. Moreover, no right-handed neutrinos are present and neutrino masses are generated radiatively with the help of a bulk charged scalar field that provides the lepton number violation. Using experimental inputs from the Global Neutrino Analysis and recent Daya Bay results, a numerical analysis is performed and allowed parameter regions are displayed.
Highlights
The Standard Model (SM) gauge group is a priori consistent with a large flavor group that is not observed experimentally, and Yukawa couplings and mixings are introduced to comply with such experimental evidence [1]
In the model we study above almost all the fields in the 4D effective action are zero modes of bulk fields; in particular, each left- and right-handed fermion has its own fivedimensional counterpart: only the Higgs fields are purely four-dimensional and live on the IR brane and, unlike the bulk fields, have no KK excitations
In order to obtain an neighbor interactions (NNI)-type quark mass matrix, we advocate the presence of a discrete symmetry upon which all fields are charged: the cyclic group Z4 is the smallest Abelian group consistent with the aforementioned texture
Summary
The Standard Model (SM) gauge group is a priori consistent with a large flavor group that is not observed experimentally, and Yukawa couplings and mixings are introduced to comply with such experimental evidence [1]. [17], we use a flavor group that reproduces the mixing matrices in both the quark and lepton sectors automatically, without the need of introducing additional flavon fields to generate nonzero entries and/or further suppressions. This makes our model more economical in terms of additional fields and more tractable, especially in the scalar sector.
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