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Manuel Masip

Publications and source records attributed to Manuel Masip.

40 records · Page 3Linked to original sources

Effects of SM Kaluza-Klein excitations on electroweak observables

The presence of an extra dimension of size R \approx TeV^{-1} introduces a tower of Kaluza-Klein gauge boson excitations that affects the standard model (SM) relations between electroweak observables. The mixing of the W and Z bosons with their excitations changes their masses and couplings to fermions. This effect depends on the Higgs field, which may live in the bulk of the extra dimension, on its boundary, or may be a combination of both types of fields. We use high-precision electroweak data to constrain 1/R. We find limits from 1 to 3 TeV from different observables, with a model independent bound of 2.5 TeV.

hep-ph↗

Leptophobic Z' from Superstring Derived Models

It was recently suggested that the reported anomalies in $R_b$ and $R_c$ can be interpreted as the effect of a heavy vector boson that couples to quarks and is universally decoupled from leptons. We examine how an extra gauge boson with this property can arise from superstring derived models. In a specific three generation model we show that the $U(1)_{B-L}$ symmetry combines with the horizontal flavor symmetries to form a universal leptophobic $U(1)$ symmetry. In our model there is an enhancement of the color gauge group from twisted sectors. The enhancement occurs after the breaking of the unifying gauge symmetry by ``Wilson lines''. The leptophobic $U(1)$ symmetry then becomes a generator of the color $SU(4)$ gauge group. We examine how similar symmetries may appear in other string models without the enhancement. We propose that if the current LEP anomalies persist it may be evidence for a certain class of un--unified superstring models.

hep-ph↗

CP violation in multi-Higgs supersymmetric models

We consider supersymmetric extensions of the standard model with two pairs of Higgs doublets. We study the possibility of spontaneous $CP$ violation in these scenarios and present a model where the origin of $CP$ violation is soft, with all the complex phases in the Lagrangian derived from complex masses and vacuum expectation values (VEVs) of the Higgs fields. The main ingredient of the model is an approximate global symmetry, which determines the order of magnitude of Yukawa couplings and scalar VEVs. We assume that the terms violating this symmetry are suppressed by powers of the small parameter $ε_{PQ}=O(m_b/m_t)$. The tree-level flavor changing interactions are small due to a combination of this global symmetry and a flavor symmetry, but they can be the dominant source of $CP$ violation. All $CP$-violating effects occur at order $ε_{PQ}^2$ as the result of exchange of {\it almost}-decoupled extra Higgs bosons and/or through the usual mechanisms with an {\it almost}-real CKM matrix. On dimensional grounds, the model gives $ε_K\approx ε_{PQ}^2$ and predicts for the neutron electric dipole moment (and possibly also for $ε'_K$) a suppression of order $ε_{PQ}^2$ with respect to the values obtained in standard and minimal supersymmetric scenarios. The predicted $CP$ asymmetries in $B$ decays are generically too small to be seen in the near future. The mass of the lightest neutral scalar, the strong $CP$ problem, and possible contributions to the $Z$ decay into $b$ quarks (the $R_b$ puzzle) are also briefly addressed in the framework of this model.

hep-ph↗

Spontaneous CP violation in supersymmetric models with four higgs doublets

We consider supersymmetric extensions of the standard model with two pairs of Higgs doublets. We study the possibility that CP violation is generated spontaneously in the scalar sector via vacuum expectation values (VEVs) of the Higgs fields. Using a simple geometrical interpretation of the minimum conditions we prove that the minimum of the tree-level scalar potential for these models is allways real. We show that complex VEVs can appear once radiative corrections and/or explicit {\it soft} CP violating terms are added to the effective potential.

hep-ph↗