Title: Trijets in Neutral Current Deep Inelastic Scattering
1Prompt Photons in Photoproduction at HERA
Preliminary Examination
Eric Brownson University of Wisconsin Jan. 13,
2005
2Outline
- 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
3Structure 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)
4Quark 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
5Quark-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
6QCD 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
7Photoproduction
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
8Jets 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
9Jets 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
10Prompt 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
11Photoproduction 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
12Photoproduction 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
13HERA 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
14HERA 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
15ZEUS Detector
16Central 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
17Uranium-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
18Barrel 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
19Online 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
20Kinematic 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
21Kinematic Reconstruction
Escapes down beam pipe
- Measured
Quantities Eh, pz, pT2
Photoproduction Topology
Luminosity Detectors
e
e
P
22Jet 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
23Jet 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
24Model 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
25Lund 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.
26Photoproduction 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
27Photoproduction 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
28Prompt Photon Event
29H1 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
30H1 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
31Previous 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
32Previous 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
33New 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
34Photoproduction Prompt g Jet Event Vertex
- Zvertex lt 55 cm
- Excludes Beam Gas Background
- Needed to accurately reconstruct the event
- PT, ET, h, etc
35Photoproduction 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
36Photoproduction 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
37Background 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
38Photoproduction 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
39Photoproduction 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
40Summary 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