The h cross section and double helicity asymmetry in pp collisions

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The cross section and double helicity asymmetry in pp collisions Frank Ellinghaus University of Colorado (for the PHENIX Collaboration) 10/03/06 Spin’06, Kyoto, Japan

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The h cross section and double helicity asymmetry in pp collisions. Frank Ellinghaus University of Colorado (for the PHENIX Collaboration) 10/03/06 Spin’06, Kyoto, Japan. Introduction. Status: A LL for h unmeasured, h fragmentation function unknown  no predictions for A LL yet - PowerPoint PPT Presentation

Transcript of The h cross section and double helicity asymmetry in pp collisions

Page 1: The  h  cross section and double helicity asymmetry in pp collisions

The cross section and double helicity asymmetry in pp collisions

Frank EllinghausUniversity of Colorado

(for the PHENIX Collaboration)10/03/06

Spin’06, Kyoto, Japan

Page 2: The  h  cross section and double helicity asymmetry in pp collisions

F. Ellinghaus, Spin’06, Kyoto, Japan

Introduction

• Status: ALL for unmeasured, fragmentation function unknown no predictions for ALL yet

• Additional channel (“global analysis”)• Naïve expectation (additional s+s in wave

function): increased relative contribution of strange quarks and glue should lead to a different asymmetry (when compared to )

• -> Observation of difference could help to disentangle the contributions from q (u,d,s) and g

22~ qaGqaGaA qqqgggLL

Access to polarized gluon distribution function via double helicity asymmetry:

Page 3: The  h  cross section and double helicity asymmetry in pp collisions

F. Ellinghaus, Spin’06, Kyoto, Japan

PHENIX Detector

Photon identification:

• EPbSC > 0.2 GeV, EPbGl > 0.2 GeV

• Cut on Shower shape of cluster• (Charge veto cut: closest track in PC3 is considered, should be far

away or very close (pair production originated from photon))• (Time-of-flight cut)

Photon detection:

• Electromagnetic calorimeter: PbSc + PbGl, Acceptance: < |0.35|, = 2 x 90

• Photon trigger: Threshold ~ 1.4 GeV

Luminosity:

• Beam-Beam Counter (BBC), 3.1 < < 4.0

Page 4: The  h  cross section and double helicity asymmetry in pp collisions

F. Ellinghaus, Spin’06, Kyoto, Japan

reconstruction via decay• Invariant two photon mass: 0.48 GeV < M < 0.62 GeV

• Energy asymmetry cut: E1-E2 / E1+E2 < 0.7

• pT > 2 GeV

• |zvertex| < 30 cm

• Fit:Gauss+Pol3

2<pT<3 GeV

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F. Ellinghaus, Spin’06, Kyoto, Japan

Invariant cross section

yp

ypN

effefffBRLppd

dE

T

T

recTrigAccT

),(1111

2

13

3

L = integrated Luminosity, based on Vernier scan using the BBC

BR= Branching ratio: 2 photons = 0.3943 ± 0.0026

fAcc = acceptance function from MC (includes smearing)

effTrig (Minimum Bias data) = Trigger efficiency of MB trigger

effTrig (high pT triggered data) = (Trigger effi. MB) x (Trigger effi. high pT

trigger)

effrec = Correct for loss due to photon conversion (~6% in PBSC, ~8% in PbGl) x loss due to cut on shower shape (~4%)

N = number of reconstructed

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F. Ellinghaus, Spin’06, Kyoto, Japan

facc from Monte CarloAcceptance and smearing correction from MC(also accounts for dead regions in EmCal, minimum cuts on photon energies,…)

Up to 10% acceptance in PbSc for at high pT

dataMC

pT

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F. Ellinghaus, Spin’06, Kyoto, Japan

Photon/MB Trigger Efficiency

Photon trigger efficiency roughly stable from 4 GeV on (high pT photon trigger threshold is set to 1.4 GeV)

Minimum Bias (MB) trigger efficiency about 80 %

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F. Ellinghaus, Spin’06, Kyoto, Japan

cross section

The relative contributions of quarks and gluons are maybe not too different…?

Need more statistics Run 5 cross section analysis in progress

Enables extraction of fragmentation functions from (e+e- and) pp ( gluon FFs)

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F. Ellinghaus, Spin’06, Kyoto, Japan

Inclusive Asymmetries

NRN

NRN

PPA

YBLL

1

L

LR Relative Luminosity R using

beam-beam counters

Asymmetries in bands around peak are consistent with each other

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F. Ellinghaus, Spin’06, Kyoto, Japan

Background corrected Asymmetry

r

ArAA

BGLL

BGLL

LL

1

BG

BG

NN

Nr

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F. Ellinghaus, Spin’06, Kyoto, Japan

Single Spin Asymmetries

NRN

NRN

PAL

1

L

LR

Parity violating asymmetries zero as expected

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F. Ellinghaus, Spin’06, Kyoto, Japan

Comparison to and Outlook

Including Run 6 data will result in statistical power comparable to present Run 5 preliminary data.

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F. Ellinghaus, Spin’06, Kyoto, Japan

Summary• Inclusive double helicity asymmetry has been extracted• Run 3 cross section for available, Run 5 result soon

enables extraction of fragmentation functions enables theoretical calculations in order to compare

extracted asymmetry to theory