Title: Production of beauty quarks in deep inelastic scattering at HERA
1Production of beauty quarks in deep inelastic
scattering at HERA
XI International Workshop on Deep Inelastic
Scattering St. Petersburg, 23-27 April 2003
2Outline
- 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
3Process topology in the ZEUS experiment
laboratory frame
(forward)
(rear)
Inner muon chambers
Central tracking detector
Outer muon chambers
4Summary 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
5Extraction 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
6Extraction 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
7Comparison with the simulation
muon variables
Good description of the event kinematics with the
extracted fractions
jet variables
8QCD 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
9Results 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
10ds/dQ2
measured at HERA for the first time!
11ds/dlog(xbj)
12NLO QCD uncertainties
- more sources
- Hadronization (jet) 10
- Fragmentation (muon) 5-10
13A tricky business...
red ICHEP02 results
14Summary 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.
15SPARE SLIDES
16Acceptance, efficiency, purity
MEPS CDM MEPS (e-p) MECCFM
17b-quark fragmentation
hep-ph/0204025
18Event 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)
19Visible 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