1 star double longitudinal spin asymmetries of inclusive charged pion production in polarized p+p...
DESCRIPTION
3 STAR Inclusive Charged Pion A LL Adam Kocoloski Measuring A LL at STAR 3 Separate Measurements Beam Polarizations Measured at RHIC polarimeters Relative Luminosities Beam-Beam Counter (BBC) scintillator tiles Spin-sorted Yields BBC and Barrel EMC trigger on events Time Projection Chamber (TPC) reconstructs and identifies pions STAR TPC | | < 1.6 and 0.5 < r < 2.0 m inside 0.5T solenoid Efficient reconstruction of charged tracks to 20 GeV; particle ID via dE/dx up to 10 GeV J. Adams, et al. Phys. Lett. B637, (2006).TRANSCRIPT
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STARSTAR
Double Longitudinal Spin Asymmetries of Inclusive Charged Pion Production in Polarized
p+p Collisions at 200 GeV
Adam Kocoloski, MITFor the STAR Collaboration
Kyoto UniversityOctober 3 2006
• Motivation
• Analysis Method
• Asymmetries
• Systematic Uncertainties
• Summary
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Why Charged Pions?
• Two complementary measurements with different contributions from polarized quark PDFs
• For qg processes, ALL(+) - ALL(-) tracks sign of G
• STAR is capable of efficient reconstruction and identification of charged pions over a large range of transverse momenta
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Measuring ALL at STAR
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ALL =σ ++ −σ +−σ ++ +σ +−
= 1P1P2
× N++ − RN+−N++ + RN+−
3 Separate Measurements
•Beam Polarizations
•Measured at RHIC polarimeters
•Relative Luminosities
•Beam-Beam Counter (BBC) scintillator tiles
•Spin-sorted Yields
•BBC and Barrel EMC trigger on events
•Time Projection Chamber (TPC) reconstructs and identifies pions
STAR TPC
•|| < 1.6 and 0.5 < r < 2.0 m inside 0.5T solenoid
•Efficient reconstruction of charged tracks to 20 GeV; particle ID via dE/dx up to 10 GeV
J. Adams, et al. Phys. Lett. B637, 161-169 (2006).
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Jet patch pTMinimum bias Jet patch
Analysis Method
Triggering•All triggers require BBC coincidence
•Statistics dominated by jet patch triggers: EM energy deposition in x = 1.0 x 1.0 patch
Cuts•Select high-quality sample of TPC tracks at || < 1.
•Particle ID accomplished using TPC dE/dx
•Use BBC timing window for vertex selection
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
2005 Inclusive +/- ALL
GRSV polarized PDFs:M. Glück, E. Reya, M. Stratmann, W. Vogelsang, PRD63, 094005 (2001).B. Jäger, M. Stratmann and W. Vogelsang, PRD70, 034010 (2004).
Fragmentation functions modified from KKP:B. A. Kniehl, G. Kramer and B. Pötter, Nucl. Phys. B582, 514 (2000).
KKP modification:Charge-separated versions of KKP pion fragmentation functions obtained by multiplying favored partons by (1+z) and unfavored by (1-z).
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Systematic Summary
Trigger Bias{3.0 - 7.3}, pT dependent
Non-longitudinal polarization 3.0
Relative Luminosity 2.2
Particle Identification 1.7
Beam Background 0.3
All uncertainties are 10-3 on ALL:
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Trigger Bias
• Majority of pions are sub-leading particles in trigger jet– Significant statistics from “away-
side”, untriggered jet as well• PYTHIA afterburner used to
construct “polarized” event generator
• Calculate ALL in simulation with and without trigger requirement
• Bias estimated using average of GRSV-min and GRSV-std scenarios
• 3.0 - 7.3 x 10-3 as a function of pT and charge sign
Other Cross-Checks• Charge-summed asymmetry
consistent with neutral pions• “Near-side” and “away-side”
asymmetries consistent with each other
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Particle ID Background
• Plot track dE/dx in terms of standard deviations from mean of pion dE/dx band
• Estimate >90% purity in acceptance window from multi-Gaussian fit
• Shift dE/dx window to select a background sample and calculate its double-spin asymmetry
• B.g. fraction x (asymmetry + 1 sigma) 1.7 x 10-3
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Looking Ahead
• 2006 saw improvements in:– polarization– – trigger acceptance and
thresholds
• Begin to look at non-inclusive measurements…
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L • dt∫
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Looking Ahead: Away-side ALL
• Calculate for each pion relative to trigger jet
• Originally motivated by trigger bias studies
– “away-side” sample free from fragmentation bias
• Reasonable statistical precision
• Needs theoretical guidance
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R = Δη( )2 + Δφ( )
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Summary• First spin result for inclusive charged pion production at STAR.
• EMC-based triggering setup limits statistics at high pT and introduces a bias in the measured ALL. This bias is estimated in simulation to be less than the size of the statistical uncertainties.
• Promising Outlook in 2006:– Significant increase in FOM– Away-side ALL reduces bias from jet trigger
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STARSTAR
Backup Slides
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Inclusive Charged Pion ALLAdam KocoloskiSTARSTAR
Comparison With Neutral Pions