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Lake Louis Winter Institute

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Study b-mesons and b-barions spectroscopy: Bs, Lb, Bc. Look for New Physics ... Time integrated ACP does not vanish at hadron colliders (since the B0B0 system ... – PowerPoint PPT presentation

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Title: Lake Louis Winter Institute


1
Recent b-physics Results from CDF
  • Giorgio Apollinari
  • Fermilab
  • for the CDF Collaboration
  • Introduction
  • CP Violation and b Mixing
  • Rare B Decays
  • Polarization in B V V
  • Future Prospects


Lake Louis Winter Institute 20-26 February 2000
2
Introduction
  • B-physics is
  • Study of the Weak Decays
  • Test the CKM Mechanism
  • Study b-mesons and b-barions spectroscopy Bs,
    Lb, Bc
  • Look for New Physics in Rare Decays
  • e.g. B0, Bs mm or em
  • Quantitative study of QCD
  • mb gtgt LQCD implies that inclusive production can
    be computed through Perturbation Theory
  • Probe gluon structure function
  • Also perform non-perturbative measurements like
    lifetimes, BF and production fractions.

3
Introduction
  • Tevatron Advantage
  • Large production
  • All b-hadron states produced
  • Bu,Bd,Bs,Bc,Lb
  • Tevatron disadvantage
  • Large Background (sin 1000 x sbb)
  • b-production peaked at low pt
  • Unknown initial state
  • Experimental Strategies
  • Specialized triggers
  • dilepton single lepton
  • J/y, y from (ee,mm) B mixing from (em, ee,
    mm),
  • b-hadron semileptonic decays
  • Precise Secondary Vertex reconstruction

4
b-physics at the Tevatron
  • Examples of Run I b-physics results from CDF

5
b-Mixing and CP Violation
  • SM with 3 generations and mixing among the quark
    families (mass eigenstates ? weak eigenstates)
    can accomodate CP violation if the complex phase
    in the unitary mixing matrix ? is ? 0?CP.
  • In the B0d,s case, like in the Ks system,higher
    order weak interactions mix meson and anti-mesons
    states.


6
b-Mixing and CP Violation
  • Unitary Triangle representation
  • from unitarity of CKM
  • S. Mele CERN-EP-98-133, 1998 sin2?0.75? 0.09
  • Parodi et al. hep-ph/9802289 sin2?0.725? 0.06
  • Ali et al. 0.52ltsin2?lt0.94

7
b-Mixing and CP Violation
  • CP violation can be manifested as
  • CP violation in the decay if A(f)/A(f) 1
  • CP violation in the mixing if the neutral mass
    eigenstates are not CP eigenstates (q/p 1)
  • CP violation in the interference between decays
    with and without mixing
  • Vtd introduces a complex phase in the box diagram
    and the interference between the two terms leads
    to a time dependent asymmetry
  • Golden mode

B0
J/y K0s
B0
8
b-Mixing and CP Violation
  • Time integrated ACP does not vanish at hadron
    colliders (since the B0B0 system is not produced
    in a coherent state)
  • PDG 98
  • A measurement of the proper time dependence of
    ACP(t) is preferable
  • more statistical power
  • reduces effect of combinatorial background at
    small t

9
b-Mixing and CP Violation
  • Measurement of ACP(t) requires 3 pieces of
    information for each decaying meson
  • Signal Reconstruction
  • Flavor of original meson
  • Use flavor tagging
  • Proper time of decay
  • Reconstruct the B vertex
  • Tagging algorithms characterized by efficiency e
    and dilution D
  • AobsCP D ACP
  • D dilution
  • NtotTotal number of events
  • NWNumber of wrong tags
  • NRnumber of right tags
  • D2P-1 (Pprob. of a ccorrect tag)
  • Best tagging has highest e D2
  • Opposite Side Lepton and/or Kaon tagging (OST)
  • Use decay of the away side B-hadron
  • Opposite Side Jet-Charge tagging
  • Reconstruct the away-side B-hadron and use
    statistical methods to determine the flavor
  • Same Side tagging (SST)
  • Uses correlation with p produced along with the
    B-hadron being tagged
  • Correlation from the B and fragmentation

10
b-Mixing and CP Violation
  • Same Side Tagging
  • uses correlation between the charge of the nearby
    p and the b quark charge due to fragmentation or
    B production
  • Gronau, Nippe, Rosner
  • p (K) tags a B0 and a p- (K-) tags a B0
  • better acceptance (efficiency) than OST
  • Track Selection
  • DRlt0.7 from B meson
  • pT gt 400 MeV
  • gt2 SVX hits
  • consistent with primary vtx in r-f and z
  • minimum prelT

B direction
PB Ptr
PB
Ptrrel
Cone ?R0.7
Ptr
11
b-Mixing and CP Violation
  • SST and mixing measurement

Mostly Charge Bs
Amplitude gives D
Mostly Neutral Bs

12
b-Mixing and CP Violation
  • First measurement of sin2b
  • F.Abe et al., Phys. Rev. Lett. 81, 5513
  • 198/- 17 B0,B0bar events
  • Asymmetry measured with SST
  • D sin2b0.31 ? 0.18 ? 0.03 (syst.)
  • D0.166 ? 0.018 ? 0.013
  • sin2b1.8 ? 1.1 ? 0.3
  • Improvements
  • candidates not fully reconstructed in SVX
  • 400 events, larger s(t)
  • Add OST
  • calibrate using B- J/y K-
  • Multiple taggers
  • use maximum L to include terms for possible
    detector biases, prompt bkg. And long-lived
    bkg.

13
b-Mixing and CP Violation
  • Signal sample in Run I

Both ? in SVX
202 ? 18 events
395 ? 31 events
S/B0.9
One or Both? not in SVX
193? 26
S/B0.7
S/B0.5
14
b-Mixing and CP Violation
  • Taggers Calibration on un-mixing B/B- samples

15
b-Mixing and CP Violation
  • Combination of flavor taggers
  • Correlations
  • Multiple tags
  • Fixing Dmd0.464?0.018 ps-1
  • Dmd floating
  • Time integrated

16
b-Mixing and CP Violation
  • Systematics
  • Dilution 0.16
  • dominated by statistic in the calibration samples
  • Others 0.02
  • Confidence Limit
  • 0ltsin 2b lt1 at 93 CL
  • if sin2b 0, the probability of observing
    sin2bgt0.79 is 3.6

17
b-Mixing and CP Violation
  • Conclusive Evidence for CP violation in B sector
  • Summary of sin 2b determinations
  • OPAL Euro. Phys. C5, 379 (98)
  • CDF(Partial) PRL 81, 5513 (98)
  • CDF(Final) hep-ex/9909003
  • ALEPH (Prelim.) BCP3 Taipei, Dec. 99
  • AVERAGE

18
Rare b Decays
  • Flavor Changing Neutral Current
  • Limits on Bo/Bs mm-
  • F.Abe et al, PRD 57, R3811 (1998)
  • Allowed by SM, 3 orders of magnitude below
    current sensistivity
  • Some SUSY models predict substantial enhancement
  • Lepton Number Conservation
  • Limits on Bo/Bs mm-
  • F.Abe et al, PRL 81, 5742 (1998)
  • Forbidden in SM
  • Sensitive to new particles (e.g. Pati-Salam
    Leptoquarks)

19
Rare b Decays
  • Non Resonant B mm K and charmless decays
  • Allowed by SM, sensitive to presence of new
    particles

20
B VV Polarization
  • Decay distributions in
  • described by 3 complex amplitudes
  • Yields CP Composition
  • - is parity-odd (L1)
  • Is a pure CP state?

21
B VV Polarization
22
Tevatron Run II B-Physics
  • CDF Upgrades
  • New Silicon Tracker, 96 cm long, r-z and r-f
    measurements
  • 2 times more acceptance
  • New dead-time-less trigger
  • Tracking information used at L1
  • Use Silicon information at L2
  • Purely hadronic B trigger possible
  • Time-of-flight
  • 2s K/p separation at plt1.6 GeV/c
  • D0 Upgrades
  • Superconducting Solenoid
  • Central Fiber Tracker
  • Silicon Microstrip Tracker

23
Tevatron Run II B-Physics
  • Precise Measurement of Vtd/Vts
  • flavor oscillation and
    , sensitive to xslt63
  • Radiative Decays
  • Precise Measurement of CP violation and sin 2b
    in
  • Observe CP violation and measure asymmetry in
  • Measure CP asymmetry in
  • Observe decay modes related to the angle g
  • Rare Decays
  • Study Bc meson and b-barions
  • Unique to Hadron Machines

24
Tevatron Run II B-Physics
  • Expectations for CP modes
  • sin 2b from B0 J/y Ks0
  • 10K reconstructed J/y Ks0
  • Taggers calibrated on
  • 40K B J/y K
  • 20K B0 J/y K0
  • eD26.7 (add 2.4 with TOF)
  • d(sin2b)0.084
  • Asymmetry in B0/B0 pp- (sin2a)
  • 8K-15K signals (if BR 10-5)
  • If signal 10K and eD2 9.1
  • dA(pp- ) 0.09
  • sin(g) modes
  • 700 events of Bs0/ Bs0 DsK

Next phase in b-physics investigation is around
the corner
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