We confront the new physics models with extra isosinglet down quarks in the new CP violation experimental era with sin(2β) and ε′/ε measurements, K+→π+ νν-events, and xs limits. The closeness of the new experimental results to the standard model theory requires us to include full standard model (SM) amplitudes in the analysis. In models allowing mixing to a new isosinglet down quark, as in E6, flavor changing neutral currents are induced that allow a Z0 mediated contribution to B-B mixing and which bring in new phases. In (p, η), (xs,sin(γ)), and (xs,sin(2φs)) plots we-still find much larger regions in the four down quark model than in the SM, reaching down to η≈0, 0≤sin(γ)≤1, -0.75≤sin(2α)≤0.15, and sin(2φs) down to zero, all at 1 σ. We el...
We review and update constraints on the parameters of the flavour mixing matrix (V_C_K_M) in the Sta...
The b quark belongs to the third generation of quarks and is the weak–doublet partner of the t quark...
In the Standard Model of particle physics, CP violation arises due to a single complex phase in the ...
We confront the new physics models with extra isosinglet down quarks in the new (Formula presented) ...
We extend the range of predictions of the isosinglet (or vector) down quark model to the fully allow...
Groups such as E6 with extra SU(2)L singlet down quarks give rise to flavor-changing neutral current...
We extend the range of predictions of the isosinglet (or vector) down quark model to the fully allow...
We review and update the constraints on the parameters of the quark flavour mixing matrix V_C_K_M in...
We impose new limits on flavor-changing neutral currents (FCNC's) applied to the 4 ± 4 mixing matrix...
I review the status of CP violation in the Standard Model from the combination of flavour constraint...
AbstractUsing primarily experimental inputs for S(Bd→ψKs), ΔMBs, ΔMBd, BR(B→τν) and ϵK along with ne...
Several new and updated BABAR measurements of sin 2β are presented, together with the latest constra...
AbstractUsing the hadronic matrix elements from the lattice, BK and ξs, involving only the 4-quark o...
We study D0 − D̄0 mixing in the presence of a fourth generation of quarks. In particular, we calcula...
We consider a model where the standard model is extended by the addition of a vector-like isosinglet...
We review and update constraints on the parameters of the flavour mixing matrix (V_C_K_M) in the Sta...
The b quark belongs to the third generation of quarks and is the weak–doublet partner of the t quark...
In the Standard Model of particle physics, CP violation arises due to a single complex phase in the ...
We confront the new physics models with extra isosinglet down quarks in the new (Formula presented) ...
We extend the range of predictions of the isosinglet (or vector) down quark model to the fully allow...
Groups such as E6 with extra SU(2)L singlet down quarks give rise to flavor-changing neutral current...
We extend the range of predictions of the isosinglet (or vector) down quark model to the fully allow...
We review and update the constraints on the parameters of the quark flavour mixing matrix V_C_K_M in...
We impose new limits on flavor-changing neutral currents (FCNC's) applied to the 4 ± 4 mixing matrix...
I review the status of CP violation in the Standard Model from the combination of flavour constraint...
AbstractUsing primarily experimental inputs for S(Bd→ψKs), ΔMBs, ΔMBd, BR(B→τν) and ϵK along with ne...
Several new and updated BABAR measurements of sin 2β are presented, together with the latest constra...
AbstractUsing the hadronic matrix elements from the lattice, BK and ξs, involving only the 4-quark o...
We study D0 − D̄0 mixing in the presence of a fourth generation of quarks. In particular, we calcula...
We consider a model where the standard model is extended by the addition of a vector-like isosinglet...
We review and update constraints on the parameters of the flavour mixing matrix (V_C_K_M) in the Sta...
The b quark belongs to the third generation of quarks and is the weak–doublet partner of the t quark...
In the Standard Model of particle physics, CP violation arises due to a single complex phase in the ...