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b physics at LEP

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two-photon events, gluon splitting, etc. New physics (CP ... but many results being superseded by pp colliders and b factories. ISMD2003. Andrea Sciab ... – PowerPoint PPT presentation

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Title: b physics at LEP


1
b physics at LEP
  • Andrea SciabĂ 
  • INFN-CNAF

XXXIII International Symposium on Multiparticle
Dynamics September 5-11, 2003 Krakow
2
b physics
  • Goals
  • CKM matrix
  • B oscillations (Vtd, Vts)
  • B semileptonic BRs (Vcb, Vub)
  • b lifetimes
  • CP violation
  • masses
  • Electroweak
  • sin2 ?W (asymmetries)
  • Rb (sensitive to new physics, mtop)
  • QCD processes
  • fragmentation
  • two-photon events, gluon splitting, etc.
  • New physics (CP violation, rare decays, etc.)

3
b physics at LEP
  • LEP data sample features and advantages
  • 3.6106 Z0 ? bb events
  • very clean environment
  • high heavy quark tagging power due to silicon
    microvertex detectors
  • production of many species of b hadrons
  • high boost of b hadrons
  • but many results being superseded by pp
    colliders and b factories

4
b physics at LEP
  • LEP data still contributes significantly to
  • b semileptonic BRs
  • Bs oscillations
  • Asymmetries, Rb (no more measurements until Z
    factories)
  • Bs, ?b, excited b hadron masses
  • Fragmentation
  • heavy quark production in 2-photon collisions
  • gluon splitting into heavy quarks
  • Only a few topics will be covered here

5
Bs oscillations
Bs oscillations Basic concepts
  • Main motivation
  • ?md ? Vtd gives a large error
  • ?md/ ?ms ? Vtd with a 3 times better
    theoretical error!
  • 15 theor. error

Bs,d0
? Vcb2
SU(3) 5 error
  • Oscillation probability
  • fit A for any assumed value ? of ?ms
  • ? ltlt?ms ? A ? 0
  • ? ??ms ? A ? 1
  • ? excluded at 95CL if A1.65sAlt1

A
6
Strategy
  • Flavour tagging at production
  • jet charges, vertex charges, kaons, leptons, etc.
  • typical mistag ? ? 25
  • Flavour tagging at decay
  • lepton or D charge
  • identify final state (b??, b?c??, etc.)
  • Distinguish Bs from other hadron species
  • Measure Bs decay length, momentum
  • ?t (m/p) ?L ? (?p/p) t
  • Maximum likelihood fit to amplitude A at given ?ms

Production flavour tagging
Decay flavour tagging
7
Oscillation analyses
  • Exclusive analyses
  • Fully reconstructed Bs (A, D)
  • Semi-exclusive analyses
  • Ds?- pairs (A, D, O)
  • Dsh- pairs (D)
  • F?- pairs (D)
  • Inclusive analyses
  • semileptonic decays (A, D, O)
  • inclusive vertices (D)

Very low statistics High purity Very high p.t.
resolution!
Low statistics Fair purity Good p.t. resolution
High statistics Low purity Low p.t. resolution
8
Fully reconstructed Bs (ALEPH)
total
Well reconstructed
Missing ?s or ?s
  • ? and ?0 reconstruction ? efficiency and purity
    increase
  • ???? ? 180 ?m??p/p? ? 0.5 3

Add a photon
?t?0.08 ps
Excellent proper time resolution!
9
Ds?- pairs (DELPHI) (updated)
Semileptonic modes
Hadronic modes
  • Event-by event
  • proper time resolution
  • Bs purity

Sensitivity ?ms 8.6 ps-1 ?ms gt 4.9 ps-1 at 95
CL
10
Inclusive ? analysis (ALEPH)
  • Topological reconstruction of the D vertex
  • Extensive event-by-event treatment of
  • proper time resolutions and corrections
  • sample composition
  • flavour tags
  • ? huge sensitivity enhancement!

Sensitivity ?ms 13.6 ps-1 ?ms gt 11.9 ps-1 at
95 CL
11
Oscillation results
  • Almost final LEP results on Bs oscillations
  • Lower limit on ?ms 14.4 ps-1
  • Now, we must wait for Tevatron to measure ?ms

12
b quark fragmentation
  • The fragmentation function models the
    non-perturbative confinement of the quark into
    colourless hadrons
  • different choices of the variablenot
    accessible experimentallyISR, FSR, hard gluon
    emission effects not unfolded
  • Model-dependent analyses (fit to a given
    fragmentation model)
  • Model-independent analyses (xB spectrum
    reconstruction)

13
Inclusive analyses
  • Event selection based on
  • b-tagging
  • secondary vertex reconstruction
  • Direct xB reconstruction (OPAL)
  • neural networks to distinguish particles from b
    decay and from hadronization
  • sE?5 GeV
  • xB, z reconstructed using neural networks
    (DELPHI), input variables correlated to
  • kinematics (track rapidity, multiplicity, etc.)
  • jet/total energy
  • b-tagging
  • preliminary

14
Exclusive analyses (ALEPH)
  • B ? D()l? decays
  • Much lower statistics
  • 3400 events
  • E? reconstructed from missing energy
  • sE 8
  • xB spectra not efficiency-corrected

15
Model dependent results
  • Favoured models
  • Lund / Lund-Bowler
  • Kartvelishvili
  • Disfavoured models
  • Peterson et al.
  • Collins

16
Model independent results
  • Mean values for xB
  • OPAL 0.71930.0016(stat.)0.0038(syst.)
  • DELPHI 0.71530.0007(stat.)0.0049(syst.)
  • ALEPH 0.7160.006(stat.)0.006(syst.)
  • All measurements consistent
  • bias w.r.t. old measurements due to
    theassumption of the Peterson model
  • -0.0033
  • -0.0052

17
AbFB measurements (I)
  • Forward-backward asymmetry at the Z pole
  • Related to sin2?W
  • AbFB most sensitive to sin2?W
  • Need to measure
  • cos? (from thrust axis)
  • quark charge
  • quark flavour
  • QCD corrections to be calculated

18
AbFB measurements (II)
  • Use a lepton tag
  • lepton charge correlated to the quark charge
  • need to distinguish
  • correct for the dilution by B mixing
  • Use the jet/vertex/kaon charge
  • b-tagging to enhance purity
  • purity from data
  • quark charge estimator Q
  • charge separation d from data
  • effect of B mixing included

19
AbFB with lepton tag (DELPHI)
New!
  • b-tagging (?EVT)
  • Track I.P., sec.vertex mass and energy, track
    rapidities
  • Flavour composition vs. ?EVT from data with
    standard double counting method
  • Lepton p and p?
  • Charge tagging
  • Lepton charge, opposite jet charge as cross check
  • Uses Q? Qopp (-/ right/wrong correlation)
  • Probability for a lepton of coming from b??,
    b?c ? ?, c ? ?, bckgnd function of (p, p?),
    (?EVT, Q? Qopp)
  • 2-dim fit of the obs asymmetry to AbFB, AcFB over
    bins of (cos?T, Pb??-Pb?c ? ?, Pc??)

20
AbFB with lepton tag (OPAL)
  • Neural networks to distinguish b?? (NETb) and c??
    (NETc)
  • Lepton p and p?, lepton jet energy, (?p?)jet
  • Jet decay length significances, lepton i.p.
    significance
  • Likelihood fit to the number of single-lepton and
    double-lepton events
  • Bins of cos?, NETb and NETc
  • Background fraction fitted from data
  • average mixing parameter ? fitted from data using
    same-sign dilepton events
  • AbFB and AcFB fitted

21
AbFB with incl. tag (DELPHI)
New!
  • high purity b-tagging (b-tag)
  • lifetime and sec vertex info, rapidities
  • b-tag selection efficiency from data counting
    events with 0,1,2 tagged hemi ? sample
    composition (b, c, uds)
  • charge tagging (flavhem)
  • jet charge, sec. vertex charge
  • flavour tag combining P(same QB) for all tracks
  • prob. of charge mistag from data
    (unlike/like-sign double tagged events)
  • for charm events, mistag from data using charge
    of reconstructed D (new!)
  • fit to no. of single and double tagged events in
    bins of (cos?, b-tag)
  • Main systematics from jet charge hem. correlations

22
AbFB with incl. tag (OPAL)
  • b events tagged with
  • NN (secondary vertex info)
  • leptons (p, p?, isolation)
  • flavour composition from data (singly and doubly
    tagged hemispheres) ? Pf
  • charge tagging estimator Q from
  • jet charge (always)
  • sec. vertex charge (if any)
  • kaon charge (from b?c ?s) (if any)
  • all charge estimators available

23
AbFB summary
  • AbFB measurements all LEP almost finalized
  • well compatible (also with SLD)
  • sin2?lepteff 2.9s discrepancy with ALR (SLD)
  • need to wait for linear colliders

SLD Ab
LEP AbFB
LEPSLD A?
24
Open b production in ?? events
  • Test of perturbative QCD
  • at LO, only direct and single resolved terms (of
    the same order)
  • more robust calculations because of the large
    quark mass
  • 2-3 orders of magnitude suppression w.r.t open
    charm because of larger mass, smaller charge
  • photons mostly quasi-real ? anti-tagged events
  • Analysis strategy
  • select anti-tagged photon-photon events
  • reconstruct lepton candidates
  • reconstruct jets
  • measure lepton p? w.r.t. jet axis
  • direct term
  • single resolved term

25
???bbX in L3
  • 627 pb-1, 189 GeV lt ?s lt 209 GeV
  • muons AND electrons ? large statistics
  • Fit to p? distribution
  • p? spectra from MC (PYTHIA for ? ?)
  • Nb, Nc, Nuds left free
  • Consistent e and ? results
  • Also measurement of
  • consistent with previous L3 results
  • muons
  • 435 events
  • electrons
  • 3850 events

26
???bbX in DELPHI (new)
  • 463 pb-1, 189 GeV lt ?s lt 209 GeV
  • only muons
  • Fit to p? distribution
  • p? spectra from MC (PYTHIA for ? ?)
  • Nc fixed to LEP average for ?(ee-?cc)
  • Nuds measured selecting hadrons instead of muons
  • Nb left free
  • Study of K-lepton correlations (first time!)
  • b?K-?-X c?K-?X
  • increased purity of c (K??) and b (K?) events
  • measured cross sections

651 events
27
???bbX in OPAL
  • 371 pb-1, 189 GeV lt ?s lt 202 GeV
  • only muons
  • Fit to p? distribution
  • p? spectra from MC (PYTHIA for ? ?)
  • Nc fixed to OPAL measurement for ?(ee-?cc) with
    D mesons
  • Nuds measured selecting hadrons instead of muons
  • Nb left free
  • xT2pT/Wvis distribution shows the consistency of
    the 11 ratio of direct to single-resolved
    contributions

444 events
28
???bb(cc) summary
  • Consistent results among LEP experiments
  • Good agreement with Drees et al. model for charm
    data
  • EXCESS for beauty data 4? discrepancy
  • No satisfactory explanation at present

29
Conclusions
  • LEP HF physics program almost finalized
  • Bs oscillations (?msgt 14.4 ps-1 at 95 CL)
  • heavy quark asymmetries (difficult
    interpretation)
  • Heavy quark fragmentation function well measured
    and consistent (both in average and shape)
  • Large discrepancy in ???bbX rate (but not in
    ???ccX rate)
  • Impossible to show many other results
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