quark mixing triangle from cp invariant and cp violating quantities

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Quark Mixing Triangle from CP Invariant and CP Violating Quantities Workshop on Neutrino Oscillations Venice , April 15-18,2008 Konrad Kleinknecht Johannes-Gutenberg Universität Mainz

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Quark Mixing Triangle from CP Invariant and CP Violating Quantities. Workshop on Neutrino Oscillations Venice , April 15-18,2008 Konrad Kleinknecht Johannes-Gutenberg Universität Mainz. Direct CP violation: ε ʹ ≠ 0 discovered by NA31(1988) ,confirmed by NA48 and kTeV. - PowerPoint PPT Presentation

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  • Quark Mixing Triangle from CP Invariant and CP Violating QuantitiesWorkshop on Neutrino Oscillations Venice , April 15-18,2008Konrad KleinknechtJohannes-Gutenberg Universitt Mainz

    NO-VE2008,Venice 15 04 08

  • Direct CP violation: 0discovered by NA31(1988) ,confirmed by NA48 and kTeVNew measurement of kTeV Re( )=(19.22.1) 10-4 confirms present (2003) value Re( )=(16.71.6) 10-4 WA shifted to (16.81.4) 10-4Conclude: Origin of CP violation comes from complex phase in quark mixing matrix a la Kobayashi- Maskawa (1973)

    NO-VE2008,Venice 15 04 08

  • NO-VE2008,Venice 15 04 08

  • Results for complex amplitudes (left side) and (right hand side)

    NO-VE2008,Venice 15 04 08

  • Direct CP- Violation exists through a complex phase in K-M-Quark Mixing2004: CP- Violation confirmed in decays of B mesons through the same mechanism. Not sufficient by far to explain baryon asymmetry of 10-9 in the universe. A much larger CP- Violation must exist somewhere else to satisfy Sacharovs criteria, maybe in the lepton sector.Through Leptogenesis an asymmetry in the lepton number could cause a quark asymmetry in a B-L conserving interactionK. Kleinknecht, Universitt MainzAverage of all experimentsResults

    NO-VE2008,Venice 15 04 08

  • Quark Mixing of 6 quarks by weak mixing K-M- matrix relates quark mass eigenstates and weak eigenstates

    NO-VE2008,Venice 15 04 08

  • Standard parametrization of KM-Matrix has 3 angles connecting generations 12 , 23 , 13, and one phase 13

    NO-VE2008,Venice 15 04 08

  • Unitarity triangleUnitarity applied to first and third column yields:

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  • New element:Observation of Bs and Bd mixingMeasurement of BOTH mixing parameters enables a new constraint on one side of the K-M-unitarity triangle:CDF and D0 obtain:Using the relation:

    And from lattice calculations :

    We obtain the constraint:

    NO-VE2008,Venice 15 04 08

  • Other CP conserving constraints K decays : Vus=0.2244 0.0022B decays: Vcb=(41.4 0.8) 10-3 Vub=(4.39 0.46) 10-3

    Vub and Vts/Vtd both yield circle-shaped range of allowed values for top of unitarity triangle

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  • CKM Unitarity triangle from CP conserving quantities

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  • CP violating constraints -- || = (2.2810.020) 10-3 from K decay -- sin2 = 0.687 0.032 from Bd(Bd)KS decay asymmetry (BaBar, Belle) -- =(99 -9+12) degrees from Bd(Bd) , , asymmetries (BaBar, Belle) yield constraints coinciding in upper half of complex plane:

    NO-VE2008,Venice 15 04 08

  • Unitarity triangle from CP violating processes

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  • All constraints togetherFit with sin sin sin

    and

    CP-phase Area of unitarity triangle

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  • Vertex of triangle from CP conservingand CP violating processes

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  • ConclusionIn the framework of the KM scheme, measurements of CP invariant quantities allow for the first time the prediction that CP violation exists with two solutionsCP violating observables determine both the same sign of the phase 13CP conserving and violating constraints agree within 2Phase 13 = + 63 4 degrees.

    NO-VE2008,Venice 15 04 08