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Philip Rubin (George Mason University)3/10/09, 5:00 PMIn the six-quark Standard Model, flavor changing due to the weak force is described by a unitary transformation represented by the 3 × 3 matrix, known as the Cabibbo-Kobayashi-Maskawa (CKM) matrix. The elements of this matrix, constrained theoretically by unitarity, must be determined experimentally. By investigating e+ e- collisions around the charm-quark threshold, the CLEO-c experiment has...Go to contribution page
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Prof. Meenakshi Narain (Brown University)3/10/09, 5:20 PMI will cover results from CDF and DZero on top quark properties, specifically the top mass, top charge, W helicity in top decays, and top anomalous couplings.Go to contribution page
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Mr Thomas Schwarz (University of California Davis USA)3/10/09, 5:40 PM
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Dr Enrique Palencia (Fermilab)3/10/09, 6:00 PMWe present the first observation of the single top quark production at the Fermilab Tevatron experiments, CDF and D0. After applying the event selection, there is a small expected signal hidden under large and uncertain backgrounds.In order to further separate signal from background events, highly sophisticated methods are needed. The results of the different analyses performed by both...Go to contribution page
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Gudrun Hiller (Dortmund)3/10/09, 6:20 PMI review opportunities from flavor physics for collider searches and b-physics.Go to contribution page
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Dr Andreas Winhart (University of Mainz)3/10/09, 6:40 PMThe SM prediction for the ratio of purely leptonic decay rates of the charged kaon $R_K=\Gamma(K_{e2}/\Gamma(K_{\mu2}))$ has an excellent sub-permille precision. Due to the helicity suppression of the SM contribution, the ratio is sensitive to non-SM effects; in particular, LFV contributions in the MSSM can modify it by a few percent without contradicting any other presently known experimental...Go to contribution page
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