8,620 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

    Bi-collinear antiferromagnetic order in the tetragonal α\alpha-FeTe

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    By the first-principles electronic structure calculations, we find that the ground state of PbO-type tetragonal α\alpha-FeTe is in a bi-collinear antiferromagnetic state, in which the Fe local moments (2.5μB\sim2.5\mu_B) are ordered ferromagnetically along a diagonal direction and antiferromagnetically along the other diagonal direction on the Fe square lattice. This bi-collinear order results from the interplay among the nearest, next nearest, and next next nearest neighbor superexchange interactions J1J_1, J2J_2, and J3J_3, mediated by Te 5p5p-band. In contrast, the ground state of α\alpha-FeSe is in the collinear antiferromagnetic order, similar as in LaFeAsO and BaFe2_2As2_2.Comment: 5 pages and 5 figure

    Inhomogeneous Diophantine approximation over the field of formal Laurent series

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    AbstractDe Mathan [B. de Mathan, Approximations diophantiennes dans un corps local, Bull. Soc. Math. France, Suppl. Mém. 21 (1970)] proved that Khintchine's theorem on homogeneous Diophantine approximation has an analogue in the field of formal Laurent series. Kristensen [S. Kristensen, On the well-approximable matrices over a field of formal series, Math. Proc. Cambridge Philos. Soc. 135 (2003) 255–268] extended this metric theorem to systems of linear forms and gave the exact Hausdorff dimension of the corresponding exceptional sets. In this paper, we study the inhomogeneous Diophantine approximation over a field of formal Laurent series, the analogue Khintchine's theorem and Jarnik–Besicovitch theorem are proved

    Fourth Generation Leptons and Muon g2g-2

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    We consider the contributions to gμ2g_\mu-2 from fourth generation heavy neutral and charged leptons, NN and EE, at the one-loop level. Diagrammatically, there are two types of contributions: boson-boson-NN, and EE-EE-boson in the loop diagram. In general, the effect from NN is suppressed by off-diagonal lepton mixing matrix elements. For EE, we consider flavor changing neutral couplings arising from various New Physics models, which are stringently constrained by μeγ\mu\to e\gamma. We assess how the existence of a fourth generation would affect these New Physics models.Comment: Minor changes, with references update
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