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Physics 222 UCSD/225b UCSB Lecture 7 Mixing & CP violation (3 of 3) Today, we focus on how to measure things, and what the present knowledge is from the.

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Presentation on theme: "Physics 222 UCSD/225b UCSB Lecture 7 Mixing & CP violation (3 of 3) Today, we focus on how to measure things, and what the present knowledge is from the."— Presentation transcript:

1 Physics 222 UCSD/225b UCSB Lecture 7 Mixing & CP violation (3 of 3) Today, we focus on how to measure things, and what the present knowledge is from the combination of theory and experiment. Take 2 sources as references: David MacFarlane at SSI 2002 Soeren Prell at Lepton-Photon 2009

2 CKM Matrix Element Magnitudes Lepton Photon 2009Expt. Status of the CKM Matrix (S.Prell)2 V ud BdBd BdBd BsBs BsBs t W D D K π π BKn p ee ee ee ν ν ν νν V us V ub V cd π ee V cs ee BdBd D ν ee V cb V td V ts V tb b

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10 Why does this matter? Heavy Quark Symmetry predicts that the B -> D* transition in B -> D* l nu has trivial form factor for the part of phase space when the D* is at rest in the B restframe. However, this also leads to minimal pT for the slow pion in the D* -> D pi decay. |V cb | is theoretically most accurately extracted from experimental data where it is experimentally most difficult.

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12 Luminosity accumulated by Belle reached 1000/fb on November 29th 2009.

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22 β from b →(cc) s decays Lepton Photon 2009Expt. Status of the CKM Matrix (S.Prell)22 Theor. clean measurement of |S| = sin2β with B → J/ψ K 0, J/ψ K*, ψ(2S)K S, η c K S, & χ c1 K S by BaBar and Belle BaBar, PRD 79,072009 (2009) statistically limited

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25 Lepton-photon 2009 Dalitz analysis now clearly dominates the precision.

26 Poluektov @ EPS’09 Basic idea: b -> u transition with c-bar quark from virtual W interferes with b -> c transition, IFF one chooses a decay of the D meson that is common for D and anti-D meson. The resonance structure then provides the CP conserving “phase analyzer” to measure gamma from the interference.

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29 Global CKM Fit Consistency of angles Consistency of angles and sides from global fit –Overall good fit (CKMFitter: global p-value 45%) –~2σ tension between sin2β and ε K / V ub correction to ε K will make it worse (Buras, Guadagnoli, PRD78, 033005 (2008)) Lepton Photon 2009Expt. Status of the CKM Matrix (S.Prell)29 CKM angles Other constraints All constraints

30 Future directions Ever more precise measurement of: –sin2  from J/  K s –  from Dalitz analysis Measurements of processes that only occur at 2nd order weak interaction in standard model –B -> s l+ l- –B -> s nu nubar Measurements of helicity suppressed decays –B to mu+mu- CP violation in the B s system

31 β s from B s → J/ψ Ф decays Lepton Photon 2009Expt. Status of the CKM Matrix (S.Prell)31 New physics in B s B s mixing CDF/PHYS/BOTTOM/CDFR/9787, DØ Note 5928-CONF D0 and CDF measure β s with angular dependent fit to decay time distributions of B s → J/ψ Ф –Simultaneous fit for ΔΓ s and β s SM predicts β s very small (~0.02) –sensitive to new physics in B s mixing Prospects –D0 and CDF working on updates with 2x samples –LHCb sensitivity with 0.5 fb -1 : σ(β s ) = 0.02

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