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We show that it is possible to accommodate the observed size of the phase in $B^0_s$--$bar B^0_s$, mixing in the framework of a model with violation of $3times 3$ unitarity. This violation is associated to the presence of a new $Q=2/3$ isosinglet quark $T$, which mixes both with $t$ and $c$ and has a mass not exceeding 500 GeV. The crucial point is the fact that this framework allows for $chiequivarg(-V_{ts}V_{cb}V_{tb}^*V_{cs}^*)$ of order $lambda$, to be contrasted with the situation in the Standard Model, where $chi$ is constrained to be of order $lambda^2$. We point out that this scenario implies rare top decays $tto cZ$ at a rate observable at the LHC and $|V_{tb}|$ significantly different from unity. In this framework, one may also account for the observed size of $D^0$--$bar D^0$ mixing without having to invoke long distance contributions. It is also shown that in the present scenario, the observed size of $D^0$--$bar D^0$ mixing constrains $chi^primeequivarg(-V_{cd}V_{us}V_{cs}^*V_{ud}^*)$ to be of order $lambda^4$, which is significantly smaller than what is allowed in generic models with violations of $3times 3$ unitarity.
The problems linked with the extraction of the basic parameters of the hadron elastic scattering amplitude at the LHC are explored. It is shown that one should take into account the saturation regime which will lead to new effects at the LHC.
The CP asymmetry predicted by the Standard Model in the decay modes Bs;d -> J/psi eta and Bs -> J/psi phi is very small, and the observation of a sizeable e ect would be a clear indication of new physics beyond the Standard Model. Contrary to the fin
We review the prospects for B decay studies at the LHC.
We review three recent results of the CDF collaboration on Bs suppressed decays: the first search for CP--violation in the Bs-->phi phi decay, where two CP--violating asymmetries expected to be zero in the Standard Model are measured, and the observa
We discuss lepton charge asymmetries in $t bar t$ and $t bar t gamma$ production at the LHC, which can be measured in the semileptonic decay channel $t bar t to W^+ b , W^- bar b to ell^+ u b , q bar q bar b$ (or the charge conjugate). Considering s