24,308 research outputs found

    Flavor and CP Violation with Fourth Generations Revisited

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    The Standard Model predicts a very small CP violation phase sin2ΦBsSM0.04\sin2\Phi^{\rm SM}_{B_s} \simeq -0.04%= \arg M_{12} \simeq \arg\,(V^*_{ts}V_{tb})^2in in B_s--\bar B_smixing. mixing. %, i.e. of order \lambda^2\eta.Anyfinitevalueof. Any finite value of \Phi_{B_s}measuredattheTevatronwouldimplyNewPhysics.Withrecenthintsforfinite measured at the Tevatron would imply New Physics. With recent hints for finite \sin2\Phi_{B_s},experimentsattheTevatron,wereconsiderthepossibilityofa4thgeneration.Asrecentdirectsearchboundshavebecomeconsiderablyheavierthan300GeV,wetakethe, % have appeared from CDF and D\O\, experiments at the Tevatron, we reconsider the possibility of a 4th generation. As recent direct search bounds have become considerably heavier than 300 GeV, we take the t'masstobeneartheunitarityboundof500GeV.Combiningthemeasuredvaluesof mass to be near the unitarity bound of 500 GeV. Combining the measured values of \Delta m_{B_s}with with {\cal B}(B \to X_s\ell^+\ell^-),togetherwithtypical, together with typical f_{B_s}values,wefindasizable values, we find a sizable \sin2\Phi^{\rm SM4}_{B_s} \sim -0.33.Using. Using %a typical value of m_{b'} = 480GeV,weextracttherange GeV, we extract the range % a range of values, 0.06 < |V_{t'b}| < 0.13fromtheconstraintsof from the constraints of \Gamma(Z\to b\bar b),, \Delta m_{D}and and {\cal B}(K^+\to\pi^+\nu\bar\nu).Afuturemeasurementof. A future measurement of {\cal B}(K_L\to\pi^0\nu\bar\nu)willdetermine will determine V_{t'd}$.Comment: 8 pages, 11 figure

    Complementarity of Semileptonic BB to K2(1430)K_2^*(1430) and K(892)K^*(892) Decays in the Standard Model with Fourth Generation

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    The BK2(1430)l+lB\rightarrow K_{2}^{\ast}(1430)l^{+}l^{-} (l=μ,τ)(l=\mu,\tau) decays are analyzed in the Standard Model extended to fourth generation of quarks (SM4). The decay rate, forward-backward asymmetry, lepton polarization asymmetries and the helicity fractions of the final state K2(1430)K^{*}_{2}(1430) meson are obtained using the form factors calculated in the light cone sum rules (LCSR) approach. We have utilized the constraints on different fourth generation parameters obtained from the experimental information on KK, BB and DD decays and from the electroweak precision data to explore their impact on the BK2(1430)l+lB\rightarrow K_{2}^{\ast}(1430)l^{+}l^{-} decay. We find that the values of above mentioned physical observables deviate deviate significantly from their minimal SM predications. We also identify a number of correlations between various observables in BK2(1430)l+lB\rightarrow K_{2}^{\ast}(1430)l^{+}l^{-} and BK(892)l+lB\rightarrow K^{\ast}(892)l^{+}l^{-} decays. Therefore a combined analysis of these two decays will compliment each other in the searches of SM4 effects in flavor physics.Comment: 28 pages, 12 figure

    Window on Higgs Boson: Fourth Generation bb^\prime Decays Revisited

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    Direct and indirect searches of the Higgs boson suggest that 113 GeV mH\lesssim m_H \lesssim 170 GeV is likely. With the LEP era over and the Tevatron Run II search via ppˉWH+Xp\bar p \to WH+X arduous, we revisit a case where WHWH or ZH+ZH + jets could arise via strong bbˉb^\prime\bar b^\prime pair production. In contrast to 10 years ago, the tight electroweak constraint on tt^\prime--bb^\prime (hence tt^\prime--tt) splitting reduces FCNC bbZb^\prime\to bZ, bHbH rates, making bcWb^\prime\to cW naturally competitive. Such a "cocktail solution" is precisely the mix that could evade the CDF search for bbZb^\prime\to bZ, and the bb^\prime may well be lurking below the top. In light of the Higgs program, this two-in-one strategy should be pursued.Comment: 4 pages, RevTex, 4 eps figures, One more figure, version to be published in Phys. Rev.

    Four Statements about the Fourth Generation

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    This summary of the Workshop "Beyond the 3-generation SM in the LHC era" presents a brief discussion of the following four statements about the fourth generation: 1) It is not excluded by EW precision data; 2) It addresses some of the currently open questions; 3) It can accommodate emerging possible hints of new physics; 4) LHC has the potential to discover or fully exclude it.Comment: Summary of the "Beyond the 3-generation SM in the LHC era" Workshop, CERN, September 4-5, 2008; 7 pages. V2: updated bibliography and minor typos fixed. To appear in PMC Physics

    Direct CP Violation in Angular Distribution of BJ/ψKB\to J/\psi K^{*} Decays

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    We show that the study of certain observables in the angular distribution in BJ/ψKB\to J/\psi K^* provide clear test for CP vioaltion beyond the Standard Model. These observables vanish in SM, but in models beyond SM some of them can be large enough to be measured at B factories.Comment: 7 pages, Revte

    Electroweak Beautygenesis: From b {\to} s CP-violation to the Cosmic Baryon Asymmetry

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    We address the possibility that CP-violation in BsBˉsB_s-\bar B_s mixing may help explain the origin of the cosmic baryon asymmetry. We propose a new baryogenesis mechanism - "Electroweak Beautygenesis" - explicitly showing that these two CP-violating phenomena can be sourced by a common CP-phase. As an illustration, we work in the Two-Higgs-Doublet model. Because the relevant CP-phase is flavor off-diagonal, this mechanism is less severely constrained by null results of electric dipole moment searches than other scenarios. We show how measurements of flavor observables by the D0, CDF, and LHCb collaborations test this scenario.Comment: 4 pages, 1 figure, 1 tabl
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