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Related papers: Strong CP, Up-Quark Mass, and the Randall-Sundrum …

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Randall-Sundrum scenario with all the standard model (SM) fermions and gauge bosons in the bulk is phenomenologically studied. Even though the simple assumption of universal bulk fermion mass m_\psi leads to the same Kaluza-Klein (KK) mass…

High Energy Physics - Phenomenology · Physics 2009-11-07 C. S. Kim , J. D. Kim , Jeong-hyeon Song

We study top quark Kaluza-Klein (KK) mode mixing in the Randall-Sundrum scenario with all the SM fermions and gauge bosons in the bulk. Even though the simple assumption of universal bulk fermion mass m_psi leads to the same KK mass…

High Energy Physics - Phenomenology · Physics 2009-11-07 C. S. Kim , J. D. Kim , Jeonghyeon Song

The version of the higher-dimensional Randall-Sundrum (RS) model with matter in the bulk, which addresses the gauge hierarchy problem, has additional attractive features. In particular, it provides an intrinsic geometrical mechanism that…

High Energy Physics - Phenomenology · Physics 2009-11-11 G. Moreau , J. I. Silva-Marcos

We propose a Randall-Sundrum model with a bulk family symmetry based on the double tetrahedral group, T', which generates the tri-bimaximal neutrino mixing pattern and a realistic CKM matrix, including CP violation. Unlike 4D models where…

High Energy Physics - Phenomenology · Physics 2014-11-20 Mu-Chun Chen , K. T. Mahanthappa , Felix Yu

We suggest the fermion doubling for all quarks and leptons. It is a generalization of the neutrino doubling of the seesaw mechanism. The new quarks and leptons are $SU(2)$ singlets and carry the electromagnetic charges of their lighter…

High Energy Physics - Phenomenology · Physics 2010-11-01 Sanghyeon Chang , Jihn E. Kim

We study quark mass matrices in the Randall-Sundrum (RS) model with bulk symmetry $SU(2)_L \times SU(2)_R \times U(1)_{B-L}$. The Yukawa couplings are assumed to be within an order of magnitude of each other, and perturbative. We find that…

High Energy Physics - Phenomenology · Physics 2008-11-26 We-Fu Chang , John N. Ng , Jackson M. S. Wu

We propose a solution to the strong CP problem that specifically relies on massless quarks and has no light axion. The QCD color group $SU(3)_c$ is embedded into a larger, simple gauge group (grand-color) where one of the massless, colored…

High Energy Physics - Phenomenology · Physics 2024-08-22 Ravneet Bedi , Tony Gherghetta , Keisuke Harigaya

It is shown that in the scheme with a rotating fermion mass matrix (i.e. one with a scale-dependent orientation in generation space) suggested earlier for explaining fermion mixing and mass hierarchy, the theta-angle term in the QCD action…

High Energy Physics - Phenomenology · Physics 2011-01-27 J. Bordes , H. M. Chan , S. T. Tsou

The Randall-Sundrum model with gauge fields and fermions in the bulk has several attractive features including the gauge coupling unification, a candidate for the dark matter, and an explanation for the hierarchical Yukawa couplings. In…

High Energy Physics - Phenomenology · Physics 2007-05-25 Hiroto Nakajima

In these proceedings we present the main results for particle-antiparticle mixing and rare decays in the Randall-Sundrum (RS) model with custodial symmetry. To investigate the strong bound on the Kaluza-Klein (KK) mass scale M_KK>O(20)TeV…

High Energy Physics - Phenomenology · Physics 2010-11-02 Bjoern Duling

The quark and charged lepton masses and the angles and phase of the CKM mixing matrix are nicely reproduced in a model which assumes SU(3)xSU(3) flavour symmetry broken by the v.e.v.'s of fields in its bi-fundamental representation. The…

High Energy Physics - Phenomenology · Physics 2008-11-26 I. Masina , C. A. Savoy

The effective action of the radion in the Randall-Sundrum model is analysed. Fine tunings are needed to obtain the observed mass hierarchy and an invisible radion. since the kinetic terms are important for determining the radion mass, the…

High Energy Physics - Theory · Physics 2009-11-07 Ian G Moss , Wade Naylor

We consider a Randall-Sundrum model in which the Standard Model fermions and gauge bosons correspond to bulk fields. We show how the observed charged fermion masses and CKM mixings can be explained, without introducing hierarchical Yukawa…

High Energy Physics - Phenomenology · Physics 2008-11-26 Stephan J. Huber , Qaisar Shafi

Scenarios seeking to address the issue of electroweak symmetry breaking often have heavy colored gauge bosons coupling preferentially to the top quark. Considering the bulk Randall-Sundrum as a typical example, we consider the prospects of…

High Energy Physics - Phenomenology · Physics 2024-04-09 Debajyoti Choudhury , Kuldeep Deka , Lalit Kumar Saini

I discuss the suppression of the lightest generation fermion mass terms in realistic superstring standard--like models in the free fermionic formulation. The suppression of the mass terms is a consequence of horizontal symmetries that arise…

High Energy Physics - Phenomenology · Physics 2009-10-22 Alon E. Faraggi

In this talk I review the `puzzles' associated with the fermion mass matrices and describe some recent attempts to resolve them, at least partially. Models which attempt to explain the observed mass hierarchy as arising from radiative…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. S. Babu

We study signals at the Large Hadron Collider (LHC) for Kaluza-Klein (KK) excitations of the electroweak gauge bosons in the framework with the Standard Model (SM) gauge and fermion fields propagating in a warped extra dimension. Such a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kaustubh Agashe , Hooman Davoudiasl , Shrihari Gopalakrishna , Tao Han , Gui-Yu Huang , Gilad Perez , Zong-Guo Si , Amarjit Soni

One of the historical suggestions to tackle the strong CP problem is to take the up quark mass to zero while keeping $m_d$ finite. The $\theta$ angle is then supposed to become irrelevant, i.e. the topological susceptibility vanishes.…

High Energy Physics - Lattice · Physics 2018-04-18 Julien Frison , Ryuichiro Kitano , Norikazu Yamada

A bonus of the framed standard model (FSM), constructed initially to explain the mass and mixing patterns of quarks and leptons, is asolution (without axions) of the strong CP problem by cancelling the theta-angle term $\theta_I$ $Tr…

High Energy Physics - Phenomenology · Physics 2022-01-05 José Bordes , Hong-Mo Chan , Sheung Tsun Tsou

Different approaches to the fermion mass problem are reviewed. We illustrate these approaches by summarizing recent developments in models of quark and lepton mass matrices. Dynamical calculations of the top quark mass are discussed, based…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. D. Froggatt
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