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Cano Ay , Johannes Gutenberg Universität , ayc@uni-mainz.de

Selected B-physics at D Ø. for the D Ø Collaboration 09 nov 2005 Flavour in the era of the LHC CERN. Tevatron and D Ø Results and Prospects DG s / G s B s Mixing B s  mm Summary. Cano Ay , Johannes Gutenberg Universität , ayc@uni-mainz.de. Tevatron. Highest Luminosity at D Ø :

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Cano Ay , Johannes Gutenberg Universität , ayc@uni-mainz.de

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  1. Selected B-physics at DØ for the DØ Collaboration 09 nov 2005 Flavour in the era of the LHC CERN • Tevatron and DØ • Results and Prospects • DGs/Gs • Bs Mixing • Bsmm • Summary Cano Ay , Johannes Gutenberg Universität , ayc@uni-mainz.de

  2. Tevatron Highest Luminosity at DØ: 1.6ּ1032 cm-2s-1 Recorded Luminosity: 1.04 fb-1 Delivered Luminosity: 1.24 fb-1 Integrated Luminosity per Experiment: ~2 fb-1 until 2006 ~8 fb-1 until 2009 Flavour in the era of the LHC , Cano Ay

  3. DØ Detector SMT H-disks SMT F-disks SMT barrels Tracking system: Coverage: ||<3.2 2T Solenoid Field • Muon system: Coverage: ||<2 Good shielding 2T Toroid Field 1m Flavour in the era of the LHC , Cano Ay

  4. Muon triggers • single inclusive muons, • ||<2.0, pT>3,4,5 GeV • Muon + track match at Level 1 and a muon at Level 2 • Unbiased; prescaled or turned off depending on inst. Lumi. • At Level 3 also invariant mass track selections (imply impact parameter bias) • Dimuons Flavour in the era of the LHC , Cano Ay

  5. Motivation Bd Mixing Bd & Bs Mixing Tevatron currently only place to study Bs Meson • SM predicts a Dms0 and DGs0 • Dms/Dmd constrain unitarity triangle larger uncertainties! smaller uncertainties! Flavour in the era of the LHC , Cano Ay

  6. Motivation • Expectation for lifetime difference DGs/Gs (with experimental input) • Discrepancies to SM Expectation  new physics • decay Bs   : example indirect search for New physics • FCNC process  highly suppressed in SM • Observing the decay would indicate new physics (SUSY, MSSM, etc) Flavour in the era of the LHC , Cano Ay

  7. B-physics program at DØ • Reconstruction of Lb in semileptonic Decays • Reconstruction of BsDsX decays • Reconstruction of B Hadron Signals at D0 • Evidence of BsDs(2536)X • Observation of the Bc Meson and study of ist properties • Study of exited B Mesons (B**) • A high statistics measurement of the Bs0 lifetime • Observation of Bs(2s) and a measurement of B(Bs(2s) ))/B( Bs(2s) ) • Search for Bs rare decays • FCNC charm decays and Observation of Ds • Bs mixing with BsDsX, Ds and opposite-side flavor tagging • Bs mixing with BsDsX, DsK*K and opposite-side flavor tagging • Flavor oscillations in Bd Mesons with 3 combined Taggers • Measurement of upsilon differential cross section • Measurement of the ratio B+ and B0 meson lifetimes • Measurement of the Lb lifetime in the decay J/yL decays • Measurement of the Bs lifetime in the exclusive decay channel BsJ/ • Measurement of the lifetime difference in the Bs system • Measurement of the semileptonic branching fractions of B mesons to narrow D** states • Observation and Properties of the X(3872) Decayoing to J/+- Flavour in the era of the LHC , Cano Ay

  8. DGs/Gs • Bs Mixing • Bsmm Flavour in the era of the LHC , Cano Ay

  9. DGs/Gs Analysis • Reconstruct • the polarisation state of the vector mesons in the final states are different for CP eigenstates • Simultaneous fit to Flavour in the era of the LHC , Cano Ay

  10. DGs/Gs Results DØ : 450pb-1 Flavour in the era of the LHC , Cano Ay

  11. Prospects DGs/Gs • Analysis improvement • Fit all 3 angles in transversity, not only 1 angle • update silicon Layer 0 • extrapolate forwards to higher luminositiy Flavour in the era of the LHC , Cano Ay

  12. DGs/Gs • Bs Mixing • Bsmm Flavour in the era of the LHC , Cano Ay

  13. Bs Mixing: Analysis Signal selection: 1. reconstructed side opposite side 2. 3. • Flavor at time of production • (Flavor tagging): • lepton charge • secondary vertex Jet charge • D²=(1.940.140.09)% Semileptonic decays: (trigger on ) Proper decay time: Flavour in the era of the LHC , Cano Ay

  14. DØ Bs Mixing Limit Limit for both channels • very large semileptonically decaying sample (~34k) in 610pb-1 • after flavour tagging (~4.2k) Flavour in the era of the LHC , Cano Ay

  15. Prospects Dms • more data • General Analysis improvements • hadronic channel, other semileptonic channels • Event-by-event fit, not binned likelihood • improved flavour tagging • Upgrades • layer 0 silicon, improved vertex resolution • L3 bandwidth 50Hz to 100Hz Dms sensitivity Flavour in the era of the LHC , Cano Ay

  16. Bs Mixing • DGs/Gs • Bsmm Flavour in the era of the LHC , Cano Ay

  17. Search for rare decay Bs Signal background • ‘blind’ analysis with 300 pb-1 • Signal selection was optimized with random grid search Flavour in the era of the LHC , Cano Ay

  18. Search for rare decay Bs • After selection 4.31.2 background events were expected and 4 events were found in the signal region • Calculate BR Limit using the B+J/K+ as normalisation channel Flavour in the era of the LHC , Cano Ay

  19. Prospects Bs • Based on DØ results at ~300pb-1 • Scale to higher luminositiy • Bands indicate 10% variation of events Flavour in the era of the LHC , Cano Ay

  20. Summary • Currently Tevatron is the best place to study Bs Meson • Presented three preliminary results (only fraction of B-physics program at DØ) • Lifetime difference DGs/Gs • Mass difference Dms (only semileptonic) • rare decay Bs with more statistics error will be reduced by a factor ~10 With improved analysis, upgrades and more data push sensitivity above the SM expectation Not sensitiv for SM Prediction, but maybe for new physics Flavour in the era of the LHC , Cano Ay

  21. Backup Flavour in the era of the LHC , Cano Ay

  22. Transversity Flavour in the era of the LHC , Cano Ay

  23. Combined Likelihood Flavour in the era of the LHC , Cano Ay

  24. Proper decay length Flavour in the era of the LHC , Cano Ay

  25. K*K data sample untagged tagged Flavour in the era of the LHC , Cano Ay

  26. Limits , K*K Limit only for Flavour in the era of the LHC , Cano Ay

  27. Disciminating variables Bs Flavour in the era of the LHC , Cano Ay

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