Mixing at the B- Factories Daniel Marlow Princeton University Beauty 2003 10/16/03 the “Iron City”

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Presentation transcript:

Mixing at the B- Factories Daniel Marlow Princeton University Beauty /16/03 the “Iron City”

Neutral B Oscillations Flavor decomposition: Time propagation: Effective Hamiltonian matrix:

Standard Assumptions Eigenvalues: If CPT is a good symmetry: Expected to be small in the SM and often taken to be ~0

... Neutral B Oscillations Eigenvectors: Indirect CP violation:

Dilepton Mixing At the B-Factories the B 0 ’s are produced in pairs such that The study of like- and opposite-sign dileptons provides a conceptually and experimentally simple way to observe the mixing, which is sensitive to Δm Same flavor: Opposite flavor:

... Dilepton Mixing The relative populations of the same-flavor and opposite-flavor samples as well as the time dependence are important. The measurement is characterized by high statistics. Belle: 29.4 fb -1 PRD In addition to Δm d, the measurement yields information on charged to neutral B production.

Other Measurements of Δm d A variety of other techniques can be used to extract Δm d. “Tag” (exclusively reconstructed)

Other Measurements of Δm d MixedUnmixed BaBar: 23M B-pairs hep-ex/ submitted to PRD

Other Measurements of Δm d Belle & BaBar Combined

Other Measurements of Δm d All experiments combined. Δm d is now very well measured!

More Dileptons One can also search for CP violation in the mixing by looking for an asymmetry in the number of like-sign dileptons: In SM effects are expected to be small.

CP & T Violation in Dileptons background signal Like-sign dilepton Δz distribution. 23M B-pairs

CP & T Violation in Dileptons 23M B-pairs PRL (2002)

Thinking the unthinkable: CPT Violation The mixing analysis can be extended to incorporate possible CPT violating effects via the inclusion of the parameter θ. If CPT is a good symmetry θ=π/2.

Thinking the unthinkable: CPT Violation Belle did a second fit to their dilepton data, allowing for the possibility of CPT violation. Belle: 29.4 fb -1 N.Hastings et al.PRD

Coherent Time Evolution at the Y(4S) B-Flavor Tagging Exclusive B Meson Reconstruction Vertexing & Time Difference Determination PEP-II (SLAC) BaBar W.Verkerke EPS2003

BaBar W.Verkerke EPS2003 hep-ex/ Time dependent B decay rates allowing  0, CP/T/CPT violation BaBar has introduced a new parameterization wherein a fit is done to samples of the form Fit to whereand

BaBar 82 fb -1 hep-ex/ Time dependent B decay rates allowing  0, CP/T/CPT violation: fit results

The Future: Δm d Single Measurement Errors Method(s)StatisticalSystematic* Now (30 fb -1 ) Dilepton±0.008±0.010 “Hadronic”±0.016±0.010 Future (300 fb -1 ) Dilepton±0.003±0.004 ~ ±0.007 “Hadronic”±0.005±0.005 ~ ±0.007 We are nearing the end of the road, but a ~twofold improvement may still be in the cards. *Systematic error projections from C.Bozzi CKM Workshop CERN 2002

The Future: CPT Parameters BaBar (82 fb -1 ) Im(z) = ± ± Re(z) = ± ± Belle (29 fb -1 ) Im(cosθ) = 0.03 ± 0.01 ± 0.03 Re(cosθ) = 0.00 ± 0.12 ± 0.02 Once again, there is room for some improvement, but we are bumping up against systematic errors. We shouldn’t forget the possibility of new ideas!