PHENIX Transverse-Spin Physics

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Presentation transcript:

PHENIX Transverse-Spin Physics Korea-Japan PHENIX Collaboration Workshop November 27, 2012 Yuji Goto (RIKEN/RBRC)

Hierarchy in Nature Glashow’s ouroboros Interaction and (breaking of) symmetry Status and structure of the material Gap between “quark & gluon” and “constituent quark” Chiral-symmetry Confinement Cosmology High-energy elementary particle physics Astrophysics Quark-gluon physics Hadron physics Nuclear physics November 27, 2012

Quark-Gluon Physics Constituent-quark model Explains the magnetic moment of the nucleon But, the quark spin cannot explain the nucleon spin “Spin Puzzle” (or “Spin Crisis”) Quark-gluon model (and QCD) Understanding of gluon interaction Chiral-symmetry Confinement Understanding of the nucleon structure Initial state of high-energy hadron collider (i.e. LHC) Orbital angular momentum Gluon spin contribution Quark spin contribution November 27, 2012

Spin Puzzle Longitudinal-spin physics x Helicity structure of the nucleon 1-dimensional Collinear factorization Incoherent scattering of partons momentum fraction in longitudinal direction x: Bjorken’s x (xBj) Parton distribution in longitudinal direction x 1/3 valence quark sea November 27, 2012

Spin Puzzle Transverse-spin physics Transverse structure of the nucleon 3-dimensional Many-body correlation of partons Parton distribution in transverse direction Extended/generalized picture of parton distribution Transverse-momentum dependence (TMD) Space distribution (tomography) Phenomenological model with GPD data Lattice QCD calculation November 27, 2012

Transverse-spin physics Single transverse-spin asymmetry Expected to be small in hard scattering at high energies FNAL-E704 Unexpected large asymmetry found in the forward-rapidity region Development of many models based on perturbative QCD xF = 2pL/s (Feynman’s x) November 27, 2012

Transverse-polarization runs at RHIC Year s [GeV] Recorded PHENIX STAR Pol [%] 2001 (Run 2) 200 0.15 pb-1 15 2003 (Run 3) / 0.25 pb-1 30 2005 (Run 5) 0.16 pb-1 0.1 pb-1 47 2006 (Run 6) 2.7 pb-1 8.5 pb-1 57 62.4 0.02 pb-1 53 2008 (Run8) 5.2 pb-1 7.8 pb-1 45 2011 (Run11) 500 25 pb-1 48 2012 (Run12) 9.2/4.3 pb-1 22 pb-1 61/58 November 27, 2012

Single transverse-spin asymmetries at RHIC Forward rapidity 0 at STAR at s = 200 GeV Forward identified particles at BRAHMS +  Forward rapidity 0 at PHENIX at s = 62.4 GeV K p November 27, 2012

Transverse-spin physics kT,p p Perturbative-QCD models Sivers effect Sivers distribution (initial state) Collins effect Transversity distribution (initial state) + Collins fragmentation (final state) Higher-twist effect Many-body correlation of quarks and gluons Sivers effect on TMD (transverse-momentum dependent) factorization Transverse structure of the nucleon Spin-orbit correlation LS force inside the nucleon Higher-twist effect on collinear factorization Parton reaction Sivers effect SP p Sq kT,π Collins effect November 27, 2012

TMD distribution and transversity u-quark u-quark d-quark d-quark Sivers function: correlation between nucleon transverse spin and parton transverse momentum (kT) Transversity: correlation between nucleon transverse spin and parton transverse spin Boer-Mulders function: correlation between parton transverse spin and parton transverse momentum (kT) November 27, 2012

Transverse-spin physics How to distinguish Sivers effect Collins effect Higher-twist effect pT distribution Need more statistics To find 1/pT at high pT STAR s = 500 GeV PHENIX s = 200 GeV November 27, 2012

MPC at PHENIX Muon Piston Calorimeter EM calorimeter installed in the small cylindrical hole in muon magnet piston PbWO4 crystals 2.22.218 cm3 22.5 cm radius 43.1 cm depth 3.1 < || < 3.9 November 27, 2012

MPC at PHENIX 0  No strong s dependence from 19.4 GeV to 500 GeV Flavor-dependence information November 27, 2012

Midrapidity asymmetries 0 and  gluon+gluon & gluon+quark dominant at low pT Restriction to Gluon Sivers effect Single electron Open heavy-flavor decay to electron/positron Restriction to tri-gluon correlation To be improved with VTX Transversity measurement with IFF (interference fragmentation function) Pion (or hadron) pair as an analyzer November 27, 2012

Forward neutron asymmetry PHENIX Collision Point ~1800cm ±2.8mrad 10cm blue beam yellow beam SOUTH ZDC Dx magnet NORTH ZDC ZDC trigger ZDC + SMD ZDC (Zero-Degree Calorimeter) Hadron sampling calorimeter SMD (Shower Maximum Detector) Position measurement xF distribution Significant negative AN in the forward region No xF dependence within the uncertainties No significant backward asymmetry ZDCBBC trigger arXiv:1209.3283 [nucl-ex] November 27, 2012

Forward neutron asymmetry s dependence of pT distribution AN(62 GeV) < AN (200 GeV) < AN (500 GeV) s dependence or pT dependence? Sensitivity to presence of different mechanisms, e.g. Reggeon exchanges with spin-non-flip amplitude, even if they are small amplitudes Inclusive neutron Neutron with charged particles PHENIX preliminary data J. Phys. Conf. Ser. 295, 012097 (2011). November 27, 2012

Spin physics in the future MPC-EX Pre-shower detector in front of MPC Silicon mini-pad detectors with tungsten plates Approved by BNL and DOE to be ready for 2015 run November 27, 2012

Spin physics in the future MPC-EX Prompt photon asymmetry To distinguish Sivers effect and higher-twist effect Collins asymmetry in jet 0 correlations with jet-like clusters 49pb-1, P=0.6 Twist-3 p+p prediction SIDIS (TMD) p+p prediction Phys Rev. D 83 094001 (2011) arXiv 1208.1962v1 (2012) AN xF Charged clusters with >=3 tracks, single-track p0’s November 27, 2012

Spin physics in the future (Forward) sPHENIX Sivers asymmetry in Drell-Yan process Competitive program in the world Comparison with Semi-Inclusive DIS measurement ePHENIX at eRHIC Polarized electron+proton collision 3-dimensional space distribution measurement (tomography) inside the proton with deeply-virtual measurements of Compton scattering (DVCS) and meson production Drell-Yan process DIS process November 27, 2012

Spin physics in the future November 27, 2012

Summary Transverse-spin physics To understand 3-dimensional parton structure of the nucleon Many-body correlation of quarks and gluons To solve the “spin puzzle” origin of the nucleon spin: orbital angular momentum Sivers effect / Collins effect / Higher-twist effect pT distribution measurement Single transverse-spin asymmetries at PHENIX Forward asymmetry with MPC and MPC-EX (2015-) Midrapidity asymmetry Forward neutron asymmetry Transverse-spin physics will have a high priority as a goal of the RHIC-Spin project November 27, 2012

Longitudinal-polarization runs at RHIC Year s [GeV] Recorded PHENIX Recorded STAR Pol [%] 2002 (Run 2) 200 / 0.3 pb-1 15 2003 (Run 3) 0.35 pb-1 27 2004 (Run 4) 0.12 pb-1 0.4 pb-1 40 2005 (Run 5) 3.4 pb-1 3.1 pb-1 49 2006 (Run 6) 7.5 pb-1 6.8 pb-1 57 62.4 0.08 pb-1 48 2009 (Run9) 500 10 pb-1 39 14 pb-1 25 pb-1 55 2011 (Run11) 27.5 / 9.5pb-1 12 pb-1 2012 (Run12) 30 / 15 pb-1 82 pb-1 50/54 November 27, 2012

Semi-Inclusive DIS asymmetry M. Anselmino, et al. EPJA 39, 89 (2009) Measurement of Sivers asymmetry and Collins asymmetry Sivers function u-quark d-quark November 27, 2012