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Trijets in Neutral Current Deep Inelastic Scattering

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Prompt Photons, Eric Brownson, U. Wisconsin. Preliminary Exam, January 13, 2005 - 1 ... h: Planck's Constant. Q: Related to the Probe's Momentum ... – PowerPoint PPT presentation

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Title: Trijets in Neutral Current Deep Inelastic Scattering


1
Prompt Photons in Photoproduction at HERA
Preliminary Examination
Eric Brownson University of Wisconsin Jan. 13,
2005
2
Outline
  • Introduction
  • HERA and ZEUS
  • Kinematics
  • Prompt Photon Events
  • Related Experimental Results
  • MC Generation and Usage
  • Event Sample and Cuts
  • Summary and Plan for the Future

3
Structure Of The Proton
  • Studied via Probe Exchange
  • Wavelength of probe l h/Q
  • h Plancks Constant
  • Q Related to the Probes Momentum
  • A smaller wavelength means greater resolution
  • HERA Collisions
  • Ee27.5 GeV , Ep920 GeV
  • HERA provides ep collisions with CMS Energy
    300 GeV
  • Provides g or W/Z as probes
  • Deep Inelastic Scattering (DIS) Q2 lt 40,000
    GeV2
  • Probe to .001 fm (Proton is 1 fm)

4
Quark Parton Model
  • Hadrons particles that interact strongly
  • Bound states of structure-less particles (quarks)
  • Quark-parton model
  • Quark properties mass, electric charge, spin
  • Quarks treated as point-like, non-interacting

5
Quark-Parton Model
  • Proton contains only valence quarks
  • Partons considered point-like particles
  • Structure functions describing individual
    particles momenta distribution depend only on
    xBj
  • No Q2 dependence (Bjorken scaling)
  • fi(x) ? Parton density functions (PDFs)
  • Must be experimentally determined

6
QCD and Colored Gluons
  • Problems with Quark-Parton Model
  • Statistics for Fermion D
  • D comprised of 3 u quarks
  • Violation of Exclusion principle under QPM
  • Sum rule for F2
  • If QPM correct
  • Value of integral shown to be 0.5 by experiment
  • Quarks carry roughly half proton momentum
  • Single quarks never observed
  • Quantum Chromodynamics gluons with color quantum
    number
  • D quark composition uRuBuG
  • Mediator of strong force ? gluon
  • Gluons carry roughly half proton momentum
  • Observed particles colorless ? color
    conservation
  • Isolated quarks not observed ? Confinement

7
Photoproduction
Direct
Resolved
  • Photon is almost real
  • Photon carries very little 4-momentum
  • Photoproduction (Q2 0)
  • DIS (Q2 gtgt 0)
  • Most ep events are Photoproduction
  • Cross section has a (1/Q4) dependence
  • Direct Photoproduction Photon couples to a
    parton
  • Resolved Photoproduction Photon fluctuates into
    Partonic State

8
Jets and Hadronization
Struck Parton ? Jet
  • Colored Partons produced in the interaction ?
    Parton Level
  • Colorless Hadrons form via hadronization ?
    Hadron Level (Fragmentation)
  • Collimated spray of particles ? Jets
  • Particle showers observed as energy deposits in
    detectors ? Detector Level

9
Jets in Resolved Direct Photoproduction
For direct and resolved either a quark or a gluon
strikes out of the proton This struck quark or
gluon will hadronize and form a jet
  • Direct Photoproduction
  • ?Virtual photon scatters off of one of the quarks
  • This leads to a sensitivity to the quark
    distribution
  • Resolved Photoproduction
  • ?A quark or gluon from the resolved virtual
    photon strikes a gluon from the proton
  • ?This leads to a sensitivity to
  • the gluon distribution

10
Prompt Photons
Prompt
  • Prompt
  • g is produced at the initial interaction point
  • ? Carries information about the struck parton
  • No Hadronization
  • Background
  • Radiative Events, The photon is radiated after
    the interaction
  • Neutral Mesons, The photon originates from a
    decay of s hadron

Radiative
11
Photoproduction of Prompt g Jet
  • Presence of a jet ?
  • Allows the underlying QCD process in the gp
    interaction to be identified more clearly
  • Presence of the prompt photon ?
  • Provide information about the underlying parton
    process that is relatively free of hadronization
    uncertainties
  • We have NLO calculations for the process
  • Closely tied to ltKTgt of the partons

12
Photoproduction of Prompt g Jet
  • When we combine prompt photons and Jets
  • We get knowledge about the hard scatter from
    jets
  • We get the clean measurement of the Photon
  • No non-perturbative hadronization of the photon
    as opposed to dijets
  • Transverse energy measurements of
    electromagnetic showers have smaller experimental
    uncertainties than for jets
  • More straightforward handle on quark and gluon
    distributions
  • In particular the h distribution of the prompt
    photon is sensitive to the quark density of the
    proton
  • We have NLO calculations for the interaction

13
HERA Description
  • 820/920 GeV Protons
  • 27.5 GeV e- or e
  • CMS Energy 300/318 GeV
  • Equivalent to 50 TeV fixed target
  • 220 bunches
  • Not all filled
  • 96 ns crossing time
  • Currents
  • 90mA protons
  • 40mA positrons
  • Instantaneous Luminosity
  • 1.8x1031cm-2s-1

H1
ZEUS
DESY Hamburg, Germany
H1 ZEUS are general purpose detectors
14
HERA Luminosity
  • Total Integrated Luminosity from 92 ? 00 193
    pb-1
  • Total From 02 ? 04 84 pb-1
  • Plan for
  • 05-07
  • 0.5 fb-1

15
ZEUS Detector
16
Central Tracking Detector
e
p
Side View
View Along Beam Pipe
  • Cylindrical Drift Chamber inside 1.43 T Solenoid
  • Measures event vertex
  • Vertex Resolution
  • Transverse (x-y) 1mm
  • Longitudinal (z) 4mm

17
Uranium-Scintillator Calorimeter
h 0.0 q 90.0o
h 1.1 q 36.7o
h -0.75 q 129.1o
h 3.0 q 5.7o
h -3.0 q 174.3o
Hadronic (HAC) Cells
Electromagnetic (EMC) Cells
Pseudorapidity
  • Depleted Uranium and Scintillator
  • 99.8 Solid Angle Coverage
  • Energy Resolution (single particle test beam)
  • Electromagnetic
  • Hadronic
  • Measures energy and position of final state
    particles

18
Barrel Presampler
  • As a a particle moves from the interaction point
    it passes through dead material in front of the
    BCAL
  • This leads to energy loss and particle decay
    before measurement
  • BCAL Presampler measurement
  • 416 Channels, one in front of each EMC/HAC tower
  • Each channel has 2X5mm thick plates of
    scintillator
  • Measured energy is proportional to the number of
    photons, not the energy of the individual photons

19
Online Event SelectionZEUS Trigger
  • 10 MHz crossing rate, 100 kHz Background rate,
    10Hz physics rate
  • First level Use data subset 10 MHz ? 500 Hz
  • Dedicated custom hardware
  • Pipelined without deadtime
  • Global and regional energy sums
  • Isolated m and e recognition
  • Track and vertex information
  • Second level Use all data 500 Hz ? 100 Hz
  • Calorimeter timing cuts
  • E pz lt 55 GeV
  • Energy, momentum conservation
  • Vertex information
  • Simple physics filters
  • Commodity transputers
  • Third level Use full reconstruction information
  • 100 Hz ? lt 10 Hz
  • Processor farm
  • Full event information
  • Refined jet and electron finding

20
Kinematic Variables
  • Center of Mass Energy of ep system squared
  • s (pk)2 4EpEe
  • Center of Mass Energy of gp system squared
  • W2 (qp)2
  • Photon Virtuality (4-momentum transfer squared at
    electron vertex)
  • q2 -Q2 (k-k)2
  • Fraction of Protons Momentum carried by struck
    quark
  • x Q2/(2pq)
  • Fraction of es energy transferred to Proton in
    Protons rest frame
  • y (pq)/(pk)
  • Variables are related
  • Q2 sxy

21
Kinematic Reconstruction
Escapes down beam pipe
  • Measured
    Quantities Eh, pz, pT2

Photoproduction Topology
Luminosity Detectors
e
e
P
22
Jet Finding Cone Algorithm
  • Maximize total ET of hadrons in cone of Fixed
    size
  • Procedure
  • Construct seeds (starting positions for cone)
  • Move cone around until a stable position is found
  • Decide whether or not to merge overlapping cones
  • Issues
  • Overlapping
  • Seed Energy threshold
  • Infrared unsafe s? 8 as seed threshold ? 0

For the Jet
23
Jet Finding Longitudinally Invariant KT Algorithm
  • In ep kT is transverse momentum with respect to
    beamline
  • For every object i and every pair of objects i, j
    compute
  • di E2T,i (distance to beamline in momentum
    space)
  • dij minE2T,i,E2T,jDh2 Df2 (distance
    between objects)
  • Calculate min di , dij for all objects
  • If (dij/R2) is the smallest, combine objects i
    and j into a new object
  • If di is the smallest, then object i is a jet
  • Advantages
  • No ambiguities (no seed required and no
    overlapping jets)
  • kT distributions can be predicted by QCD

24
Model Events PYTHIA Generator
  • Parton Level
  • LO Matrix Element Parton Shower
  • Hadron Level Model
  • Fragmentation Model
  • Lund String (Next Slide)
  • Detector Level
  • Detector simulationbased on GEANT

Parton Level
Hadron Level
Detector Simulation
Factorization Long range interactions below
certain scale absorbed into protons structure
25
Lund String Fragmentation
  • color "string" stretched between q and q moving
    apart
  • confinement with linearly increasing potential
    (1GeV/fm)
  • string breaks to form 2 color singlet strings,
    and so on., until   only on-mass-shell hadrons.

26
Photoproduction Observables Xgmeas
Xgmeas Fraction of the Photons momentum
involved in the collision
  • Direct Photoproduction Xg 1
  • Resolved Photoproduction Xg lt 1

Xpmeas Fraction of the Protons momentum
involved in the collision
27
Photoproduction Observables P-
  • Momentum Imbalances of the photon relative to the
    jet
  • Linked to the intrinsic momentum of the struck
    parton ltKTgt

Xgmeasgt0.9
T
Y
g
X
jet
28
Prompt Photon Event
29
H1 Prompt Photons in Photoproduction hg
Measurement of Prompt Photon Cross Sections in
Photoproduction at HERA DESY Preprint 04-118
  • NLO calculation describes data better
  • Factor of just under 2 for the two cases
  • Same qualitative shape

30
H1 Prompt Photons in Photoproduction ETg
Measurement of Prompt Photon Cross Sections in
Photoproduction at HERA DESY Preprint 04-118
  • Factor of just under 2 for the two cases
  • Same qualitative shape
  • Large errors associated with g Jet

31
Previous ZEUS Prompt Photons in Photoproduction
Study of the effective transverse momentum of
partons in the proton using prompt photons in
photoproduction at HERA Physics Letters B 511
(2001) 19-32
  • Photons with negative rapidity are of interest
  • The errors are statistical

32
Previous ZEUS Prompt Photons in Photoproduction
Study of the effective transverse momentum of
partons in the proton using prompt photons in
photoproduction at HERA Physics Letters B 511
(2001) 19-32
ltKTgt (GeV)
Xgmeasgt0.9
T
  • ? Gives K0 1.42 GeV
  • The errors are largely statistical

33
New ZEUS Prompt g Jet Photoproduction Analysis
  • Trigger Cuts
  • FLT
  • EMC Energies gt Threshold
  • Total Cal. Energy gt Threshold
  • At least one good Track
  • SLT
  • Zvtx lt 60 cm
  • E-Pz gt Threshold
  • ET(Box) gt 8.0 GeV
  • TLT
  • Limit on the Number of Bad Tracks
  • At least one electron from the elec5 electron
    finder with,
  • ETggt4.0 GeV , -3.0lthglt1.5
  • Offline Cuts
  • Zvtx lt 55 cm
  • No Scattered electron
  • ? Selects Photoproduction Events
  • 0.2 lt YJB lt 0.8
  • ?Lower Remove Beam Gas
  • ?Upper Remove DIS Events
  • Photon Jet
  • Hadronic Jet
  • If Two Hadronic Jets are found the One with
    higher ET is used

34
Photoproduction Prompt g Jet Event Vertex
  • Zvertex lt 55 cm
  • Excludes Beam Gas Background
  • Needed to accurately reconstruct the event
  • PT, ET, h, etc

35
Photoproduction Prompt g Jet Ymeas
  • 0.2 lt Ymeas lt 0.8
  • Y gt 0.2,
  • Eliminate proton gas background
  • Eliminate cosmic events
  • Y lt 0.8,
  • ?Eliminate DIS events
  • i.e. Events where the photon is actually a
    misidentified electron

36
Photoproduction Prompt g Jet Energy Deposit
Ratio
  • Separating the photon and hadronic Jet
  • Photons deposit almost all of their energy in
    the EMC section of the CAL
  • Hadronic jets deposit more of their energy in
    the HAC section of the CAL than photons

37
Background Neutral Mesons
Background
Solution Barrel Presampler
  • BPRE signal lt 7 (mips)
  • Reject events where the photon interacted with
    dead material
  • Reject events with more photons

38
Photoproduction Prompt g Jet ETg, hg
Photon Hadronic Jet found with the Kt Jet
Finder Photon cuts Eemc/Etot gt 0.9 -0.74 lt hg lt
1.1 ETg gt 5 GeV Hadronic jet cuts Eemc/Etot lt
0.9 -1.6 lt hg lt 2.4 ETjet gt 6 GeV
39
Photoproduction Prompt g Jet ETjet, hjet
Photon Hadronic Jet found with the Kt Jet
Finder Photon cuts Eemc/Etot gt 0.9 -0.74 lt hg lt
1.1 ETg gt 5 GeV Hadronic jet cuts Eemc/Etot lt
0.9 -1.6 lt hg lt 2.4 ETjet gt 6 GeV If 2 jets were
found the one with the highest ET was used
40
Summary Plan
  • Summary
  • Photoproduction of prompt photon jet provides
    a clean well described sample with sensitivity to
    quark gluon distributions
  • They provide a means of measuring ltKTgt for
    partons
  • BPRE provides a means of background separation
    independent of the photon energy (Commissioned in
    98)
  • Plan
  • Analyze new high luminosity sample
  • Examine disagreement with model for forward jets
  • Systematic error study
  • Ymeas Lower cuts on jet and photon ET are of
    particular importance
  • Calculate ltKTgt for partons
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