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Related papers: Exploring the Quark Flavour Puzzle within the 3 Hi…

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In this paper, we discuss the multi-Higgs doublet models, that could be effectively induced by the extended Standard Model (SM). In particular, we focus on the phenomenology in the supersymmetric model with left-right (LR) symmetry, where…

High Energy Physics - Phenomenology · Physics 2019-01-09 Syuhei Iguro , Yu Muramatsu , Yuji Omura , Yoshihiro Shigekami

A $SU(3)_Q \times SU(3)_u \times SU(3)_d$ invariant scalar potential breaking spontaneously the quark flavour symmetry can explain the standard model flavour puzzle. The approximate alignment in flavour space of the vacuum expectation…

High Energy Physics - Phenomenology · Physics 2015-03-06 Enrico Nardi

A simple breaking of the subnuclear democracy of the quarks leads to a mixing between the second and the third family, in agrement with observation. Introducing the mixing between the first and the second family, one finds an interesting…

High Energy Physics - Phenomenology · Physics 2007-05-23 Harald Fritzsch

We consider an extension of the Standard Model in which the symmetry is enlarged by a global flavour factor A4 and the scalar sector accounts for three copies of the Standard Model Higgs, transforming as a triplet of A4. In this context, we…

High Energy Physics - Phenomenology · Physics 2015-03-17 Reinier de Adelhart Toorop , Federica Bazzocchi , Luca Merlo , Alessio Paris

We propose a tri-hypercharge (TH) embedding of the Standard Model (SM) in which a separate gauged weak hypercharge is associated with each fermion family. In this way, every quark and lepton multiplet carries unique gauge quantum numbers…

High Energy Physics - Phenomenology · Physics 2026-02-17 Mario Fernández Navarro , Stephen F. King

It is known that a three Higgs doublet model (3HDM)symmetric under an exact $A_4$ symmetry is not compatible with nonzero quark masses and/or non-block-diagonal CKM matrix. We show that a 3HDM with softly broken $A_4$ terms in the scalar…

High Energy Physics - Phenomenology · Physics 2023-05-03 Iris Bree , Sergio Carrolo , Jorge C. Romao , Joao P. Silva

The results of an extensive flavour physics analysis in the Littlest Higgs model with T-parity are presented. In particular, mixing and CP-violation in K^0 and B^0_{d,s} systems have been studied. Several scenarios defined by the values of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Cecilia Tarantino

We reconsider the flavor problem in the models with two Higgs doublets. By studying two generation toy models, we look for flavor basis independent constraints on Yukawa couplings that will give us the mass hierarchy while keeping all…

High Energy Physics - Phenomenology · Physics 2011-03-17 Andrew E. Blechman , Alexey A. Petrov , Gagik Yeghiyan

This review considers models with extended Higgs sectors in which there are tree-level flavor-changing neutral currents (FCNC) mediated by scalars. After briefly reviewing models without tree-level FCNC, several models with such currents…

High Energy Physics - Phenomenology · Physics 2022-10-05 Marc Sher

The gauge sector of the Standard Model (SM) exhibits a flavour symmetry which allows for independent unitary transformations of the fermion multiplets. In the SM the flavour symmetry is broken by the Yukawa couplings to the Higgs boson, and…

High Energy Physics - Phenomenology · Physics 2013-05-29 Th. Feldmann , M. Jung , Th. Mannel

Consequences of a specific class of two Higgs doublet models in which the Higgs induced tree level flavour changing neutral currents (FCNC) display minimal flavour violation (MFV) are considered. These FCNC are fixed in terms of the CKM…

High Energy Physics - Phenomenology · Physics 2008-11-26 Anjan S. Joshipura , Bhavik P. Kodrani

The charged fermion mass matrices are always invariant under $U(1)^3$ symmetry linked to the fermion number transformation. A class of two Higgs doublet models (2HDM) can be identified by requiring that the definition of this symmetry in an…

High Energy Physics - Phenomenology · Physics 2010-12-24 Anjan S. Joshipura , Bhavik P. Kodrani

We argue that flavour mixing, both in the quark and charged lepton sector, is basically determined by the lightest family mass generation mechanism. So, in the chiral symmetry limit when the up and down quark masses vanish, all the quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. L. Chkareuli , C. D. Froggatt

The multi-Higgs models having spontaneous CP violation (SPCV) and natural flavor conservation (NFC) lead to a real CKM matrix $V$ contradicting current evidence in favour of a complex $V$. This contradiction can be removed by using a…

High Energy Physics - Phenomenology · Physics 2009-01-16 Anjan S. Joshipura , Bhavik P. Kodrani

When the Higgs doublets in the 3HDM transform as a flavor triplet of the $A_4$ group, the lepton mass matrices accommodate the experimental neutrino mixing angles at arbitrary precision while maintaining the correct mass ordering of the…

High Energy Physics - Phenomenology · Physics 2025-12-12 Bartosz Dziewit , Marek Zrałek , Joris Vergeest

We propose a viable minimal model with spontaneous CP violation in the framework of a Two Higgs Doublet Model. The model is based on a generalised Branco-Grimus-Lavoura model with a flavoured $\mathbb{Z}_2$ symmetry, under which two of the…

High Energy Physics - Phenomenology · Physics 2019-10-02 Miguel Nebot , Francisco J. Botella , Gustavo C. Branco

Flavour symmetries in the dark sector are a theoretically motivated and phenomenologically appealing concept. The dark matter particle can be stabilised with the help of flavour symmetries, without the need to introduce an additional…

High Energy Physics - Phenomenology · Physics 2015-08-26 Monika Blanke

We propose a scenario which accommodates all the masses and mixings of the SM fermions in a model of warped extra-dimensions with all matter fields in the bulk. In this scenario, the same flavor symmetric structure is imposed on all the…

High Energy Physics - Phenomenology · Physics 2015-06-19 Mariana Frank , Cherif Hamzaoui , Nima Pourtolami , Manuel Toharia

QCD lattice simulations with 2+1 flavours (when two quark flavours are mass degenerate) typically start at rather large up-down and strange quark masses and extrapolate first the strange quark mass and then the up-down quark mass to its…

QCD lattice simulations with 2+1 flavours typically start at rather large up-down and strange quark masses and extrapolate first the strange quark mass to its physical value and then the up-down quark mass. An alternative method of tuning…

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