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Event Shape Variables in Deep Inelastic Scattering at HERA

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Title: Event Shape Variables in Deep Inelastic Scattering at HERA


1
  • Event Shape Variables in Deep Inelastic
    Scattering at HERA
  • Preliminary Examination
  • Adam Everett
  • Outline
  • Introduction
  • HERA and ZEUS
  • Deep Inelastic
    Scattering
  • Jets
  • Event Shapes
  • Outlook

2
Study of Partons
  • Particle Scattering
  • Study charge magnetic moment distributions
  • Scattering via probe exchange
  • Wavelength
  • Special Case Deep Inelastic Scattering
  • High energy lepton transfers momentum to a
    nucleon via probe

h Planks Constant Q related to momentum of
photon
Size of proton 1 fm HERA can probe to
0.001 fm
3
Perturbative and Nonperturbative Regimes
  • Quantum Chromodynamics (QCD)
  • strong interactions mediated by gluon
  • Coupling as Q2 increases, ?S(Q2) decreases
  • Examine Perturbative ? Nonperturbative

4
HERA Description
  • 920 GeV p
  • 27.5 GeV e- or e
  • 318 GeV cms
  • 50 TeV Fixed Target
  • Instantaneousluminosity max 1.8 x 1031 cm-2s-1
  • 220 bunches
  • 96 ns crossing time
  • IP90mA p ?
  • Ie40mA e ?

DESY Hamburg, Germany
5
HERA Data
  • Luminosity upgrade
  • 5x increase in Luminosity
  • ? expect 1 fb-1 by end of 2006
  • Measured polarization between 60-70
  • Spin-rotators for polarized measurement

6
ZEUS Detector
7
ZEUS Angles
8
Kinematic Variables
Center of mass energy of the ?P system
Square of momentum transfer
Energy transfer to struck parton 0 ? y ? 1
(Momentum fraction of struck parton)/P 0 ?x ? 1
?s Center of mass energy
9
Kinematic Reconstruction
  • Four Measured Quantities Ee, ?, Eh, ?.

(p,E) conservation
?
?
DIS Event
10
HERA Kinematic Range
  • Q2 sxy
  • 0.1 lt Q2 lt 20000 GeV2
  • 10-6 lt x lt 0.9
  • 50 TeV Fixed Target Experiment

11
Deep Inelastic Scattering Cross Section
  • DIS Cross Section Given by Structure Functions
    F2, F1, xF3

12
DIS Event
13
Naïve Quark Parton Model
  • Scattering on proton is sum of elastic scattering
    on all of the protons constituents (partons)
  • Point-like Partons
  • Structure Functions quantify distribution of
    particles and their momentum
  • Parton Distribution Functions (PDF)
  • Must be derived from experiment

Bjorken Scaling Only x dependence
14
QCD Theory
  • Gluons vector colored bosons carry strong force
  • Gluons produce quark and gluon pairs
  • Quarks gain transverse momentum
  • Gluon-driven increase in F2
  • ?Bjorken Scaling Violation Fi(x)? Fi(x,Q2)
  • ?Observation of QCD effects

? Small x
15
Jets
  • Colored partons evolve to a roughly collinear
    spray of colorless hadrons
  • ? JETS
  • Partons gt Hadrons gt Detector schematically

As observed
As produced
16
Jet Finding
  • Uses ET and R
  • Issues seed, infrared unsafe
  • Combines jets if dij is smallest of di,dij
  • Issues none known

Cone Method
KT Method
17
Dijets
  • Direct gluon coupling
  • Opportunity to directly examine QCD effects
  • Dominant QCD diagrams for dijets

Boson Gluon Fusion
QCD Compton
18
Dijet Event
jet
jet
19
Study Jets in Breit Frame
  • The Brick Wall Frame
  • In leading order struck quark turns around
  • ? Single jet event jet has no ET
  • Dijet event jets balanced in ET
  • Breit Frame helps with multijet identification

20
Current Hemisphere of Breit Frame
DIS Event
  • e-p Breit frame
  • photon is space like
  • ?Quarks hadronization products in current
    hemisphere

Lab Frame
Breit Frame
PT
PL
Breit Frame
21
Methods to Study QCD
  • QCD Effects Gluons
  • Evolution of Quark Distributions
  • Gluons change quark distributions
  • Indirect inferred from quark distribution
  • Dijets
  • Direct gluons observed as jets
  • Complexity of jet reconstruction and
    identification
  • Event Shapes
  • Energy and particle flow
  • Direct gluon radiation changes event shapes
  • Do not need to reconstruct jets
  • Reduce dependence on hadronization

22
Event Shapes
  • Event Energy Distribution
  • Event Particle Angle Distribution
  • Define Event Shape Variables to examine (next
    slides)
  • General
  • Sphericity of the particle distribution
  • Aplanarity
  • Specific
  • Thrust
  • Broadening wrt. thrust axis
  • Out-of-Plane Momentum
  • Azimuthal Correlation

23
Sphericity
  • Describes isotropy of energy flow
  • Measure of the summed p2T wrt. Sphericity axis

24
Aplanarity
  • Describes energy flow out of Sphericity evt.
    plane
  • Measure of pT out of plane

25
Thrust in DIS
  • Linear collimation of hadronic system along a
    specified (thrust) axis
  • T interpretation depends on choice of axis
  • Four Thrusts in DIS TZ, TM, Tm, TC

TC axis
TZ axis
TM axis
Tm axis
26
Thrust and Sphericity
27
Broadening
  • Broadening of particles in transverse momentum
    wrt. thrust axis
  • ? BT, BW

28
Event Plane
  • Scattering of two objects occurs in a plane
  • Parton Model Event Plane defined by two vectors
  • Example lepton-lepton
  • Conservation of vector momentum

29
Out-of-plane Momentum
  • Energy flow out of event plane defined by proton
    direction and thrust major axis

30
Azimuthal Correlation
  • Momentum weighted function of the azimuthal angle
    around the photon-proton axis in the Breit frame
    between pairs of hadrons.

?h
?h
pth
pth
31
Sphericity and Aplanarity in ee- LEP
  • DELPHI 1993-1995, 1997
  • 243 pb-1 (6K evts.)
  • 48 lt ?s lt 189 GeV
  • Good agreement between models and data
  • Event shapes used in ee- annihilations to
    measure the running coupling

32
Thrust and Broadening at ZEUS
  • ZEUS 1995-1997
  • 48 pb-1 (321K evts.)
  • 10ltQ2lt20480 GeV2
  • 0.0006ltxlt0.6

33
Event Shape Study
  • Collect event sample for 1999 data
  • 22 pb-1 on tape
  • Extend data to 1996-2000 Sample 114 pb-1
  • Compare with theoretical Models implemented in
    Monte Carlo Simulations
  • Choose one model for first look
  • Later compare with other models
  • Improvements
  • Larger event sample
  • Improved understanding of model and data
  • Study other frames

34
Background selection Timing
35
Event Selection E-pz
36
Monte Carlo Description
37
Size and Statistics
  • Selection Cuts
  • yJB gt 0.04
  • yel lt 0.95
  • Vertex with z lt 50 cm
  • x gt 14 cm or y gt 14 cm
  • 38 lt E-pZ lt 65 GeV
  • Good positron with Eegt 10 GeV
  • First Look 1999 positron data
  • ZEUS on-tape 22 nb-1
  • Cuts ? 6476 events

cm
Monte Carlo Data
GeV
38
Sphericity and Aplanarity
  • Indicates many planar, back-to-back particles

Log plot of 0.5 to 1
Log plot of 0.1 to 0.5
Monte Carlo Data
39
Thrust
  • Indicates collimated Y particle distribution

Log plot of 0.5 to 0.65
Monte Carlo Data
40
First Look at Out-of-Plane Momentum
  • Plausible for a first pass
  • More statistics and more work to come!

Log plot of 3.5 to 15
Monte Carlo Data
41
Future Plan of Analysis
  • Enlarge event sample to full data set (96-00)
  • 114pb-1 on tape (over 140 increase over previous
    results)
  • Compare high statistic data to various models
    with Monte Carlo simulations
  • Study systematic effects

42
Conclusions
  • Study of Event Shapes in DIS at HERA
  • Should provide a powerful method to study QCD
  • Examine the connection between Perturbative and
    Nonperturbative regimes
  • Reduce dependence on hadronization and jet
    reconstruction
  • Provides a direct observation of gluon radiation
  • First look shows acceptable level of agreement
  • Larger sample available for good statistics
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