0000000001248242

AUTHOR

Joao P. Silva

showing 8 related works from this author

Looking for Delta I=5/2 amplitude components in B ->pi pi and B ->rho rho experiments

2006

We discuss how experiments measuring B -> pi pi and B -> rho rho may be used to search for a Delta I = 5/2 amplitude component. This component could be the explanation for a recent (albeit very tentative) hint from B(Bbar) -> rho rho decays that the isospin triangles do not close.

Física
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Constraining new interactions with leptonic tau decays

1995

13 páginas, 10 tablas.-- PACS number(s): 13.35.Dx, 12.60.Cn, 12.60.Fr

PhysicsCouplingHigh Energy Physics - PhenomenologyGauge bosonParticle physicsHigh Energy Physics - Phenomenology (hep-ph)Physics beyond the Standard ModelHigh Energy Physics::PhenomenologyMichel parametersFOS: Physical sciencesFísicaFermionStandard Model
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Weak magnetic dipole moments in two-Higgs-doublet models

1995

We investigate the effects of the new scalars in a two-Higgs-doublet model on the weak magnetic dipole moments of the fermions at the $Z$ peak. Proportionality of the Yukawa couplings to the fermion masses, and to $\tan{\beta}$, makes such effects more important for the third family, and potentially relevant. For the $\tau$ lepton, the new diagrams are suppressed by $v_\tau = 2 \sin^2 \theta_W - 1/2$, or by powers of $m_\tau/M_Z$, but may still be comparable to the SM electroweak contributions. In contrast, we find that the new contributions for the bottom quark may be much larger than the SM electroweak contributions. These new effects may even compete with the gluonic contribution, if the…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsElectron–positron annihilationHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaFermionBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentLepton
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Reparametrization invariance of B decay amplitudes and implications for new physics searches in B decays

2005

When studying B decays within the Standard Model, it is customary to use the unitarity of the CKM matrix in order to write the decay amplitudes in terms of only two of the three weak phases which appear in the various diagrams. Occasionally, it is mentioned that those two weak phases can be used in order to describe any decay amplitude, even beyond the Standard Model. Here we point out that, when describing a generic decay amplitude, the two weak phases can be chosen completely at will, and we study the behavior of the decay amplitudes under changes in the two weak phases chosen as a basis. Of course, physical observables cannot depend on such reparametrizations. This has an impact in discu…

FísicaHigh Energy Physics::Experiment
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Models with three Higgs doublets in the triplet representations of A4 or S4

2013

We consider the quark sector of theories containing three scalar SU(2)(L) doublets in the triplet representation of A(4) (or S-4) and three generations of quarks in arbitrary A(4) (or S-4) representations. We show that for all possible choices of quark field representations and for all possible alignments of the Higgs vacuum expectation values that can constitute global minima of the scalar potential, it is not possible to obtain simultaneously nonvanishing quark masses and a nonvanishing CP-violating phase in the Cabibbo-Kobayashi-Maskawa quark mixing matrix. As a result, in this minimal form, models with three scalar fields in the triplet representation of A(4) or S-4 cannot be extended t…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaDiscrete SymmetriesHigh Energy Physics::ExperimentMaximal CP nonconservationQuark mass matrices
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Measurements of new physics in B -> pi pi decays

2005

If new physics (NP) is present in B -> pi pi decays, it can affect the isospin I=2 or I=0 channels. In this paper, we discuss various methods for detecting and measuring this NP. The techniques have increasing amounts of theoretical hadronic input. If NP is eventually detected in B -> pi pi -- there is no evidence for it at present -- one will be able to distinguish I=2 and I=0, and measure its parameters, using these methods.

High Energy Physics - PhenomenologyFísica
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Can one detect new physics in I=0 and/or I=2 contributions to the decays B ->pi pi

2005

We study the effects of new-physics contributions to B --> pi pi decays, which can be parametrized as four new complex quantities. A simple analysis is provided by utilizing the reparametrization invariance of the decay amplitudes. We find that six quantities can be reabsorbed into the definitions of Standard Model-like parameters. As a result, the usual isospin analysis provides only two constraints on new physics which are independent of estimates for the Standard Model contributions. In particular, we show that one is not sensitive to new physics affecting the I=0 amplitudes. On the other hand, I=2 new physics can be detected, and its parameters can be measured by using independent deter…

High Energy Physics - PhenomenologyFísicaComputer Science::Databases
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Bounds on gamma from CP violation measurements in B ->pi(+)pi(-) and B ->psi K-S

2004

We study the determination of gamma from CP-violating observables in B -> pi+ pi- and B -> psi K_S. This determination requires theoretical input to one combination of hadronic parameters. We show that a mild assumption about this quantity may allow bounds to be placed on gamma, but we stress the pernicious effects that an eightfold discrete ambiguity has on such an analysis. The bounds are discussed as a function of the direct (C) and interference (S) CP-violating observables obtained from time-dependent B -> pi+ pi- decays, and their behavior in the presence of new physics effects in B-Bbar mixing is studied. (V2: Misprints corrected. Slightly improved discussion.)

FísicaHigh Energy Physics::Experiment
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