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New Results for Transverse Spin Effects at COMPASS
Anselm Vossen ALU Freiburg EINN 2007, Milos
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Agenda Short Introduction to New results from 2002-2004 data
The Compass Experiment Transverse Spin Effects at Compass New results from data Collins effect for K0 Transversity from Leading 2 Hadron Asymmetries Sivers effect for K0
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Compass Experiment (2004) high energy beam large angular acceptance
broad kinematical range beam: 160 GeV/c intensity 2·108 µ+/spill (4.8s/16.2s) two stages spectrometer Large Angle Spectrometer (SM1), Small Angle Spectrometer (SM2) tracking, calorimetry, PID MuonWall SM2 E/HCAL E/HCAL SM1 MuonWall Polarised Target or RICH m beam
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Transverse Data taken 2002 - 2004
10 Mill. DIS events transversely polarized deuteron target ~ 20% of the running time RICH PID starting 2003
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Measuring Transversity in SIDIS
_ + Collins effect m’ _ Lz-1 Lz _ + * * ? m _ + q Helicity base: independent amplitudes: _ +
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Measuring Transversity
Transversity base: Probabilistic interpretation ↑ ↓ ↑ _ _ + = _ + Difference in densities for ↑, ↓ quarks in ↑ nucleon Azimuthal SSA on Transv. Pol. nucleon
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Collins Effect in SIDIS
Ph transverse momentum of the hadron S’ transverse spin of the struck quark m’ m S’ g* FC Ph x “Collins angle” C = h - s’ z Fragmentation Function for a transversely polarised quark into unpolarised hadron spin dependent part : “Collins fragmentation function” Number of Events:
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Selection of SIDIS Events
COMPASS transverse data DIS cuts: Q2 > 1 (GeV/c)2 0.1< y < 0.9 W > 5 GeV/c2 HERMES K0 selection 2 charged particles -0.3 (GeV/c)2 < M-Mk0 < 0.3 (GeV/c)2 pt rel. to p1+p2>25 MeV/c (Armenteros plot) z > 0.2 pt/GeV/c (pl1-pl2)/(pl1+pl2)
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Collins, All Kaons
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Transversity signal in 2 Hadron Correlations
Azimuthal Asymmetry measurement similar to Collins Asymmetry extraction (z2P1+z1P2)/(z1+z2) =Ph S’ Ph F2H m m’ z x g*
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Event Selection Leading 2 Hadron
Q2>1 0.1 < y < 0.9 W > 5 GeV/c2 Leading 2h h1 leading, h2 subleading in event z1,2>0.1 (current fragmentation region) xF 1,2> 0.1 0.25 < z1+z2< (no exclusive events)
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Predictions for Expecting Signal around -Mass
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Compass Results +- - + ++ - -
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Kaon-Pion Combinations
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Like Sign Kaon Combinations
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Kaon-Kaon Combinations
K+/K-: / K-/K+: / K+/K+: / K-/K-: / f
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Sivers Effect + } x x M. Burkardt, PRD, 66, (2002)
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Sivers Effect m’ “Sivers angle” m S g* FS Ph x Modulation in FS of the hadron distribution Correlation between the nucleon spin and quark motion Sivers effect ≠0 ⇒ Quark angular momentum ≠ 0 z modulation in FS of the hadron distribution
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All K0s
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Summary/Outlook for transverse spin physics at COMPASS
So far Precise COMPASS data, identified hadrons with deuteron target available Collins and Sivers from All and Leading π+, π-, K+, K-, K0 2 Hadron Correlations from Pions and Kaons Each Combination gives new constraints on Distribution and Fragmentation functions 6 more transverse Spin dependent Asymmetries in TMD SIDIS XSection COMPASS currently measures with proton target! Flavor separation
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Backup
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Single Hadron Collins, Sivers
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Leading K0, Collins
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Leading K0
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XBj Binning
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XBj Binning
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Hadron Pairs Invariant Mass Spectra
all hadron pairs: M
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The polarised 6LiD-Target
Two 60 cm long target cells with opposite polarization Superconducting Dipole (0.5 T) 3He – 4He dilution refrigerator Vertex distribution: T=50mK Polarization: % Dilution factor: 0.38 Transverse target polarization: Reversed one a week
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Ring Imaging Cherenkov Detector
Identification of π, K and protons Cherenkov thresholds: π ≈ 3 GeV/c K ≈ 9 GeV/c p ≈ 17 GeV/c 2σ π/K separation at 43 GeV/c 6 m 5 m 3 m Radiator: C4F10 Mirror wall CsI MWPC
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Results for all hadrons
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Results beyond Collins and Sivers
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Results beyond Collins and Sivers
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Results beyond Collins and Sivers
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Particle ID in Data Hadron identification is based on RICH response: several studies performed on the stability in time of the detector. Cherenkov thresholds: π ~ 3 GeV/c K ~ 9 GeV/c p ~ 17 GeV/c 2 σ π/K separation at 43 GeV/c In the hadron sample: ~76% pions ~12% kaons
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Frame independent definition of φR
A. Baccetta, hep-ph/ where P1T and P2T are the transverse components of the hadron momenta with: we define:
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Comparison with Theory
Model calculations for COMPASS kinematics (M. Radici, QCDN 06, hep-ph/ ): Model for transversity: Soffer, Stratmann, Vogelsang, P.R. D65 (02) Korotkov, Nowak, Oganessian, E.P.J. C18 (01) 639 Schweitzer et al., P.R. D64 (01) Wakamatsu P.L. B509 (01) 59 ΔTq(x) xBj Prediction for COMPASS: small asymmetries on the deuteron ARS Mh
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Predictions for Asymmetries on the Proton
Predictions for two-hadrons asymmetries on the proton at COMPASS: Soffer, Stratmann, Vogelsang, P.R. D65 (02) Korotkov, Nowak, Oganessian, E.P.J. C18 (01) 639 Wakamatsu P.L. B509 (01) 59 - ARS (M. Radici, hep-ex/ )
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