The h cross section and double helicity asymmetry in pp collisions
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Transcript of 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
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:
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
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
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
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
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 %
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)
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
F. Ellinghaus, Spin’06, Kyoto, Japan
Background corrected Asymmetry
r
ArAA
BGLL
BGLL
LL
1
BG
BG
NN
Nr
F. Ellinghaus, Spin’06, Kyoto, Japan
Single Spin Asymmetries
NRN
NRN
PAL
1
L
LR
Parity violating asymmetries zero as expected
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.
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