Production of beauty quarks in deep inelastic scattering at HERA - PowerPoint PPT Presentation

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Production of beauty quarks in deep inelastic scattering at HERA

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XI International Workshop on Deep Inelastic Scattering. St. Petersburg, 23-27 April 2003 ... through, pions and kaons in-flight decays (cross checked with real ... – PowerPoint PPT presentation

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Title: Production of beauty quarks in deep inelastic scattering at HERA


1
Production of beauty quarks in deep inelastic
scattering at HERA
XI International Workshop on Deep Inelastic
Scattering St. Petersburg, 23-27 April 2003
2
Outline
  • Event topology
  • Event selection
  • Signal extraction and cross section calculation
  • QCD predictions and related uncertainties
  • Results total and differential cross sections
  • Comparison with other measurements
  • Summary and outlook

3
Process topology in the ZEUS experiment
laboratory frame
(forward)
(rear)
Inner muon chambers
Central tracking detector
Outer muon chambers
4
Summary of the event selection
Data sample ZEUS 1999-2000 ep (60 pb-1)
DIS cuts Q2gt2 GeV2 0.05ltylt0.7 40ltE-pzlt65 GeV box cut 12x24 cm
Muon cuts P(c2)gt1 pmgt2 GeV 30ºltqmlt160º
Jet cuts At least one jet in the Breit frame ETBreitgt6 GeV -2lthLablt2.5 Jet associated to the muon ETBreitgt4 GeV QED radiation cuts
5
Extraction of the s.l. b-decays (1)
  • After the selection cuts the data sample is a
    mixture of several processes
  • Fake muons Punch-through, Sail-through, pions
    and kaons in-flight decays (cross checked with
    real data)
  • Semi-leptonic decays of charmed hadrons
  • Semi-leptonic decays of beauty hadrons

6
Extraction of the s.l. b-decays (2)
  • 836 events after all cuts
  • Charm and light-quark ptrel distributions are
    added together according to the respective cross
    sections
  • The b-fraction is extracted with the Binned
    maximum likelihood method
  • fb (25.34.8)
  • The algorithm takes in account the statistical
    errors of the data and MC samples in each bin

210 beauty events
7
Comparison with the simulation
muon variables
Good description of the event kinematics with the
extracted fractions
jet variables
8
QCD predictions NLO calculations
  • The calculation of the NLO QCD predictions
    proceeds in three steps
  • HVQDIS (B.Harris, J.Smith, hep-ph/9503484)
    gg?bb, gg?bbg, gq?bbq, etc.
  • Fragmentation of the b-quark into a B-meson
  • Semileptonic decay of the B-meson

9
Results and QCD predictions
Measured cross section svis 38.77.7(stat.)6.1
(syst.)-5.0(syst.) pb NLO QCD (HVQDIS) sNLO
28 5.3 - 3.5 pb mR,F2 Q24mb2 mb4.75
GeV Peterson frag. function Proton parton
distribution CTEQ5F4
Model Program Cross Section (pb)
LO HVQDIS 14.4
MEDGLAP RAPGAP 17.1
CDM RAPGAP 16.3
MECCFM CASCADE 36.8
Data/NLO 1.4 but in agreement within exp. and
theoretical uncertainties
mR,F2 pT24mb2
10
ds/dQ2
measured at HERA for the first time!
11
ds/dlog(xbj)
12
NLO QCD uncertainties
  • more sources
  • Hadronization (jet) 10
  • Fragmentation (muon) 5-10

13
A tricky business...
red ICHEP02 results
14
Summary and conclusions
  • We have measured a visible cross-section of
    b-quark production in DIS and single differential
    cross-sections (Q2, xbj) for the first time at
    HERA
  • The cross section is measured with events
    containing the scattered positron, a hard jet in
    the Breit frame and a muon traversing the inner
    and outer muon chambers.
  • Detailed analysis of the theoretical uncertaities
    has been performed
  • The measured cross-section is a factor 1.4 above
    the NLO QCD predictions but in agreement within
    the experimental and theoretical uncertainties
  • Similar result in the ZEUS measurement in
    photoproduction
  • The description of the b-quark production is
    still an open question. Cannot draw a unique
    conclusion from the existing results.

15
SPARE SLIDES
16
Acceptance, efficiency, purity
MEPS CDM MEPS (e-p) MECCFM
17
b-quark fragmentation
hep-ph/0204025
18
Event simulation Monte Carlo
  • Parton shower with
  • CCFM-like evolution
  • CASCADE
  • Matrix Element with incoming off-shell gluon
  • Angular ordering in the gluon ladder
  • Direct (pointlike) component only
  • Gluon density unintegrated in kT and extracted
    from a fit to the HERA structure function F2
  • Lund string model
  • Parton shower with DGLAP Evolution
  • Matrix Element with incoming on-shell gluon
  • KT ordering in the gluon ladder
  • RAPGAP
  • Lund string model
  • Color dipole model and MEPS

...more samples generated to understand the
model dependance
Light quarks 120106 events (200 pb-1) Charm
quarks 7.5106 events (94 pb-1) Beauty
quarks 430103 events (540 pb-1)
19
Visible vs extrapolated measurements
  • Visible cross section the kinematic region is
    close to the detector acceptance
  • Example ep ? bbx ? m Jet Jet X
  • Model assumptions are not absorbed in the
    experimental result but in the corresponding QCD
    predictions ? published measurements are then
    safe
  • Extrapolated cross sections
  • Extrapolation to an unmeasured kinematic region
    the unmeasured phase space is taken from a Monte
    Carlo simulation (for example extrapolation to
    the jet or muon full phase space)
  • It is nice to quote more general and inclusive
    measurements, but...
  • Is the h and ET spectrum of the extrapolated
    region the same in the NLO as in the Monte Carlo?
  • How large are the extrapolation factors? Are they
    reported in the published results?
  • Is the extrapolation considered in the estimation
    of the systematic uncertainties?
  • Extrapolation from detector to parton/hadron
    level the corresponding correction factors are
    extracted from a Monte Carlo simulation
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