J. Hernandez-Sanchez

Yukawa textures and charged Higgs boson phenomenology in the type-III two-Higgs-doublet model

We discuss the implications of assuming a four-zero Yukawa texture for the properties of the charged Higgs boson within the context of the general two-Higgs-doublet model of type III. We begin by presenting a detailed analysis of the charged Higgs boson couplings with heavy quarks and the resulting pattern for its decays. The production of charged Higgs bosons is also sensitive to the modifications of its couplings, so that we also evaluate the resulting effects on the top decay t?bH+ as well as on “direct” cb? ?H++c.c. and “indirect” qq? ,gg?t? bH++c.c. production. A significant scope exists at the Large Hadron Collider for several H± production and decay channels combined to enable one to distinguish between such a model and alternative two-Higgs-doublet scenarios.

Flavor violating signatures of lighter and heavier Higgs bosons within the Two Higgs Doublet Model Type-III at the LHeC

We analyze the prospects for observing the light and heavy

Light charged Higgs bosons decaying to charm and bottom quarks in models with two or more Higgs doublets

CP

An effective Lagrangian description of charged Higgs decays H+→W+γ, W+Z and W+h0

-even neutral Higgs bosons (

Off-diagonal terms in Yukawa textures of the Type-III 2-Higgs doublet model and light charged Higgs boson phenomenology

\ensuremath{\phi}=h

Impact of a four-zero Yukawa texture on h → γγ and γZ in the framework of the Two Higgs Doublet Model Type III

and

Implications of the discovery of a Higgs triplet on electroweak right-handed neutrinos

H

Couplings of quarks in a partially aligned two Higgs doublet model with a four-zero texture Yukawa matrix

) in their decays into flavor violating

Update of the 2HDM-III with a four-zero texture in the Yukawa matrices and phenomenology of the charged Higgs Boson

b\overline{s}

Higgs decay into two photons from a 3HDM with flavor symmetry

channels (including charge conjugation) at the proposed Large Hadron electron Collider (LHeC), with