first measurement of the inclusive jet cross section in p+p collisions at e cm =200 gev

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Mike Miller First measurement of the inclusive jet cross section in p+p collisions at E CM =200 GeV M.L. Miller (MIT) Motivations: 1. Baseline for inclusive jet A LL 2. Constraining large-x pdf’s Outline: 1. What do we mean by “jet”? 2. Presentation of work in progress 3. List of short- and long- term tasks towards final results

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M.L. Miller (MIT). First measurement of the inclusive jet cross section in p+p collisions at E CM =200 GeV. Motivations: Baseline for inclusive jet A LL Constraining large-x pdf’s Outline: What do we mean by “jet”? Presentation of work in progress - PowerPoint PPT Presentation

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Page 1: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller

First measurement of the inclusive jet cross section in p+p collisions at ECM=200 GeV

M.L. Miller (MIT)

Motivations:

1. Baseline for inclusive jet ALL

2. Constraining large-x pdf’s

Outline:

1. What do we mean by “jet”?

2. Presentation of work in progress

3. List of short- and long-term tasks towards final results

Page 2: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

parto

n

parti

cle

etcpe

,,,

gq,

dete

ctor

What do we mean by “jet”?

Page 3: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

parto

n

parti

cle

etcpe

,,,

gq,

dete

ctor

DataData

What do we mean by “jet”?

*(hep-ex/0005012)

midpoint-cone algorithm*•Search over “all” possible seeds for stable groupings

•Check midpoints between jet-jet pairs for stable groupings

•Split/merge jets based on Eoverlap

•Add track/tower 4-momenta

Page 4: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

parto

n

parti

cle

dete

ctor

etcpe

,,,

gq,

midpoint-cone algorithm*•Search over “all” possible seeds for stable groupings

•Check midpoints between jet-jet pairs for stable groupings

•Split/merge jets based on Eoverlap

•Add track/tower 4-momenta

DataData SimulationSimulation

GEANT

“geant” jets

“pythia” je

ts

Correction philosophy•Use Pythia+GEANT to quantify detector response

•Estimate corrections to go from “detector” to the “particle” level

pyth

ia

What do we mean by “jet”?

*(hep-ex/0005012)

Page 5: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

pT (track/tower) > 0.2 GeV|vertex-z|<60 cmrcone=0.4, fmerge=0.50.2< ηjet <0.8ratio<0.9(and ET-trig>3.5 GeV/c for HT)

High Tower TriggerBBC coincidence + one tower above threshold (not the best jet trigger!)

εTrig(η=0.0)=1: ET-tower= 2.5 GeVεTrig(η=0.8)=1: ET-tower= 3.3 GeV

TPC0<φ<2π1< η<1BEMC0<φ<2π0< η<1in situ MIP+e calibration

2004 p+p data set2004 p+p run

Sampled luminosity: ~0.16 pb-1

1.4 M High tower (HT) events0.8 M highly pre-scaled minimum bias (MB) events ~220k pT>5 GeV jets in HT sample before cutsCommissioned 1x1 jet patch trigger– main jet trigger in 2005+

Page 6: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

2004 p+p runSampled luminosity: ~0.16 pb-1

1.4 M High tower (HT) events0.8 M highly pre-scaled minimum bias (MB) events ~220k pT>5 GeV jets in HT sample before cutsCommissioned 1x1 jet patch trigger– main jet trigger in 2005+

pT (track/tower) > 0.2 GeV|vertex-z|<60 cmrcone=0.4, fmerge=0.50.2< ηjet <0.8ratio<0.9(and ET-trig>3.5 GeV/c for HT)

High Tower TriggerBBC coincidence + one tower above threshold (not the best jet trigger!)

εTrig(η=0.0)=1: ET-tower= 2.5 GeVεTrig(η=0.8)=1: ET-tower= 3.3 GeV

2004 p+p data set

TPC0<φ<2π1< η<1BEMC0<φ<2π0< η<1in situ MIP+e calibration

40 200 .GeV, rs

Page 7: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Background Removal

jetT

EMCT

EE

f

:fractionenergy neutral

Datapythia+geant

Cut to remove background

Systematic uncertainty on yield from background less than ~5%

Page 8: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Consider detector response (measured) to known input (true)

trueT

measT

trueT

pppresolution :

Simulation: ~25% ± 5% for 10<pT<50 GeV/c

Consistent number derived from (modest) sample of di-jet events

“geant jets” “pythia jets”

Response & bin quality factors

Simulation

Page 9: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Consider detector response (measured) to known input (true)

“geant jets” “pythia jets”

generated

measured

NNpurity

accepted

:

jets all Of

Response & bin quality factors

Simulation

Simulation

Page 10: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Consider detector response (measured) to known input (true)

“geant jets” “pythia jets”

Bins of width 1-sigma “purity” of ~35% over range on the diagonal.

Motivates application of bin-by-bin correction factors.

Response & bin quality factors

Simulation

Simulation

generated

measured

NNpurity

accepted

:

jets all Of

Page 11: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

TacceptedMB-events dp

dNN

1

:yieldevent -per raw

Reasonable agreement between data/MC10 weighted pythia samples Slope difference:

Short term: incorporated into sys. uncertaintyLong term: iterative re-weighting of MC sample

Allows data/MC comparison before luminosity

For HT, include trigger pre-scale:

trigMB

acceptedMB-events

acceptedMB-events psNN

11

Uncorrected per-event yield

4.0 , 200 rGeVs

Page 12: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

pythia

Tpythia

geantTgeant

T pNpM

pc

MB data statistics limited

More advanced unfolding techniques currently under study

εjet : decreases c(pT)

resolution: increases c(pT)

εTrig: ~1 e-2 at pT-jet = 5 GeV ~1 at pT-jet = 50 GeV

Bin-by-bin correction factors“measured”

“true”

Simulation

resolutionpc jettriggerT :

Page 13: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Only data-statistical errors shownSystematics and ratios on next slides

Fortran code from hep-ph/0404057 (Jager et al.)rcone=0.4CTEQ 6.1μF= μR =pT

Agrees with EKS NLO to better than 1%

Towards a “corrected” cross section

TTTT dpdN

pcdtLpdpd

d

111

6.0211

±30% but invisible on this scaleMB/HT overlap for 3 bins

acceptedeventsMB

MBvertBBC

NdtL

1 ~60%

Under study

4.0 , 200 rGeVs

Page 14: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

* Under Study

* Under Study

* Under Study

•Dominant uncertainty: 10% change in ECal ~40% change in yield•More under long term study (see last slide)

Dominant systematic uncertainty estimatesNormalization

Pythia slope Statistics of c(pt) Background

BBC TriggerEnergy ScaleFr

actio

nal C

hang

e in

x-s

ectio

n

Page 15: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

“Corrected” data vs. NLO calculation

GeVs 200

40 , 200 .rGeVs

•50% systematic uncertainty from E-scale shown•Agreement (within systematics) over 7 orders of magnitude

Page 16: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

“Corrected” data vs. NLO calculationThings that could change this curve:1. Refined BEMC calibration (pi0

calibration)2. Improved correction for lost (no

vertex) events (MC embedded in abort-gap data)

3. Improved unfolding scheme

Issues that won’t go away for 2004:1. HT trigger: fragmentation bias,

slow turn on with pT-jet 2. Jet energy scale (need integrated

luminosity for photon-jet!)

GeVs 200

4.0 , 200 rGeVs

•50% systematic uncertainty from E-scale shown•Agreement (within systematics) over 7 orders of magnitude

Page 17: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

• Much work to develop methods and techniques for jet triggering, reconstruction, and analyses

• First look: – Significant pT reach (~50 GeV/c)– Agreement within large systematics with NLO calculations

• A few primary issues under study:– Refining in situ EMC calibrations (AuAu vs. CuCu vs. pp)– Overall scale corrections for no-vertex events– Improved unfolding methods– Fragmentation bias (e.g., Pythia vs. Herwig)– NLO clustering scheme

• Goal:– Bring 2004 (and 2003) analyses to efficient closure– Large 2005 data set produced, thesis analyses underway

• Long term cross section goals– Jet shapes, NLO comparisons– High stats possible improvement of large-x pdf’s

Summary and outlook

Page 18: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Backup slides

Page 19: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Charged Track Momentum p/p TPC 1% Charged Track Inefficiency 10% x 60% jet 6%*

Neutral Tower Energy Gain/Gain = 10% 40% in yield

Neutral Energy Inefficiency ∑ET from n+K0L/S+++ 6-10%*

MIP Subtraction 10% Correction to Jet ET 1%

Fiducial Detector Effects Edges/Dead regions 2% Jet calculation 1 tower = =0.05 3%Background Trigger Background trigger +MINBIAS

event5% in yield

Background Energy Jet + underlying Background 0Underlying Event Work in Progress NAFragmentation Comparison to HERWIG

ongoing NA

* Included in Correction Factor

Jet Energy Scale Systematics

Page 20: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

2004 BEMC Calibration

Typical tower response to MIP candidate in 2004 AuAu

All towers, ptrack > 1.8 GeV

Relative gain: •tower-by-tower MIP response•~250 +- 50 MeV/mip

Absolute gain:•Eta ring TPC-electrons•2<pelectron<6 GeV/c

Page 21: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Theory Systematics

Changing the pdf Changing the scale

Page 22: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Data vs. MC

Clear background for ratio>0.9Data/MC agreement improves at higher pt

Page 23: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Data vs. MC

Page 24: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Data vs. MC

Red pythia + gstarBlack dataAll error bars statistical

High tower triggerpt (jet) >10 GeV/c

Page 25: First measurement of the inclusive jet cross section in  p+p  collisions at  E CM =200 GeV

Mike Miller, for the STAR collaboration

Data vs. MC

Red pythia + gstarBlack dataAll error bars statistical

High tower triggerpt (jet) >10 GeV/c