Abstract

It is now established that the major source of electroweak symmetry breaking (EWSB) is due to the observed Higgs particle. However, whether the Higgs mechanism is responsible for the generation of all the fermion masses, in particular, the fermions of the first two generations, is an open question. In this letter we present a construction where the light fermion masses are generated through a secondary, subdominant and sequestered source of EWSB. This fits well with the approximate U(2) global symmetry of the observed structure of the flavor sector. We first realize the above idea using a calculable two Higgs doublet model. We then show that the first two generation masses could come from technicolor dynamics, while the third generation fermions, as well as the electroweak gauge bosons get their masses dominantly from the Higgs mechanism. We also discuss how the small CKM mixing between the first two generations and the third generation, and soft mixing between the sequestered EWSB components arise in this setup. A typical prediction of this scenario is a significant reduction of the couplings of the observed Higgs boson to the first two generation of fermions.

Highlights

  • The mechanism of Electroweak Symmetry Breaking (EWSB) and the generation of fermion masses are among the main frontiers of research in high energy physics

  • We explore the possibility that the above approximate U(2) structure is linked with the way EWSB is communicated to the flavor sector

  • If the sector containing Φ3 and the third generation of fermions is completely decoupled from the second source of EWSB, the observed Higgs boson would have no couplings to the light fermions

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Summary

Introduction

The mechanism of Electroweak Symmetry Breaking (EWSB) and the generation of fermion masses are among the main frontiers of research in high energy physics. If the sector containing Φ3 and the third generation of fermions is completely decoupled from the second source of EWSB, the observed Higgs boson would have no couplings to the light fermions.

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