Drell-Yan experiments at Fermilab/RHIC/J-PARC. QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN)
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1 Drell-Yan experiments at Fermilab/RHIC/J-PARC QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN)
2 Outline Fermilab Drell-Yan experiments Unpolarized program Flavor asymmetry of sea-quark distribution Boer-Mulders distribution Polarized Drell-Yan experiments Polarized Drell-Yan proposals of Fermilab program PHENIX upgrade program at RHIC Possible J-PARC program
3 Drell-Yan experiments Fixed target experiment (e.g. at Fermilab) forward detector acceptance chooses large x b and small x t x target x beam
4 Flavor asymmetry of sea-quark distribution Fermilab-E866/NuSea experiment E beam = 800 GeV (from Tevatron) x = (valence region) σ pd ~ 1 2 d ( x + 2) 1 u ( x ) pp 2σ 2 with CTEQ5M dx[ d ( x) u ( x)] = ± dx[ d ( x) u ( x)] = ± 0.012
5 Fermilab-E906/SeaQuest experiment Main Injector 120 GeV Tevatron 800 GeV Dimuon measurement from Drell-Yan process 120-GeV proton beam from the Fermilab Main Injector
6 Fermilab-E906/SeaQuest experiment Nucleon structure With hydrogen and deuterium targets Select anti-quark distributions in hadrons Flavor asymmetry of sea-quark distributions Boer-Mulders distribution Cold Nuclear Matter (CNM) With nuclear targets Partonic energy loss EMC effect
7 Flavor asymmetry of sea-quark distribution Fermilab-E906/SeaQuest experiment E beam = 120 GeV (from Main Injector) x = Blue band: MSTW function refit error band with E866 data Yellow band: error band with E866 data + E906 expected statistics
8 Flavor asymmetry of sea-quark distribution Competition between perturbative QCD gluon dissociation non-perturbative contributions Meson cloud model u g q q Chiral quark model Instanton model π + in the proton as an origin of anti-d quark pseudo-scaler meson should have orbital angular momentum in the proton
9 Drell-Yan decay angular distributions A general expression for Drell-Yan decay angular distributions λ can differ from 1, but should satisfy 1-λ=2ν (Lam- Tung relation) Reflect the spin-1/2 nature of quarks (analog of the Callan-Gross relation in DIS) Insensitive to QCD corrections Violation of the Lam-Tung relation ν 0 and ν increases with p T Violation of the Lam-Tung relation suggests new mechanisms with non-perturbative origin
10 Drell-Yan decay angular distributions Boer-Mulders function h 1 Transverse-momentum dependence of transverselypolarized partons inside the (unpolarized) nucleon Small ν is observed for p+d and p+p π - +W: [valence h 1 (π)] [valence h 1 (p)] p+d and p+p: [valence h 1 (p)] [sea h 1 (p)] L. Y. Zhu et al., Phys. Rev. Lett. 99 (2007) Phys. Rev. Lett. 102 (2009) Error profile for SeaQuest statistics
11 SeaQuest commissioning run February 22 nd April 30 th, GeV/c proton beam, 19 ns interval (53 MHz) Beam intensity: proton/spill (5 s spill at 1 minute interval) Target: H 2, empty flask, D 2, Fe, C, W Unstable beam bunch intensity Feedback control of the beam extraction magnet (accelerator group under construction) Trigger veto against high intensity bunch (prototype test)
12 Commissioning run Dimuon mass distribution Mass resolution at J/ψ peak ~0.3 GeV/c 2 almost consistent with hardware specification Improvement of the track reconstruction algorithm underway Coming physics run Main injector upgraded Extraction beam line commissioning ongoing Beam to the SeaQuest experiment late October, year data accumulation ( ) for protons on target Beam intensity: protons/spill (5s spill at 1 minute interval)
13 Polarized Drell-Yan experiment Toward understanding of the Spin Puzzle with extended picture of the nucleon structure 3-dimensional description of the nucleon structure Quantum many-body correlation of quarks and gluons Transverse quark-gluon distribution inside the nucleon TMD (Transverse-Momentum Dependence) factorization and collinear higher-twist factorization Transverse-momentum distribution inside the nucleon Single transverse-spin asymmetry Sivers function Transversity Boer-Mulders function Double transverse-spin asymmetry Transversity (quark antiquark for p+p collisions) Double helicity asymmetry Flavor asymmetry of sea-quark polarization
14 Non-universality of TMD distribution function Opposite-sign contribution of TMD distribution function to SSA in semi-inclusive DIS (SIDIS) process and Drell-Yan process SIDIS Drell-Yan Fundamental property based on gauge invariance of QCD Experimental verification required Understanding in wide kinematic range from fixed target experiments to collider experiments Polarized Drell-Yan experiments COMPASS, SeaQuest, RHIC(, GSI-FAIR, NICA, ) Polarized SIDIS experiments EIC
15 Polarized Drell-Yan experiment P1027 Polarized beam experiment May 18 th, 2012 proposal submitted November 14 th, 2012 stage-1 approval
16 Polarized Drell-Yan experiment P1027 Clean measurement of sign and shape of Sivers distributions to compare DIS and Drell-Yan POT Red curve: prediction from SIDIS data (HERMES & COMPASS)
17 Polarized Drell-Yan experiment P1039 Polarized target experiment May 6 th, 2013 LoI submitted June 26 th, 2013 stage-1 approval Polarized target R&D at LANL LANL LDRD project FY
18 RHIC
19 Detector upgrade project at PHENIX sphenix Barrel upgrade Compact jet detector Extension of tracking layers and preshower detector Forward upgrade Partial installation and commissioning in Completion and experiment in ephenix at erhic Transition to erhic in Commissioning and experiment start in 2025
20 R (cm) sphenix forward upgrade Open geometry Wide kinematic coverage of photon, jet, leptons and identified hadrons Compatible design for erhic detector (ephenix) Constraint from IR design of erhic ( z < 4.5m) Hermeticity for exclusive measurements η~1 R (cm) η~-1 HCal HCal MuID EMCal Central silicon tracking EMCal& Preshower RICH η~4 Silicon Station1 GEM Station2 GEM Station3 GEM Station4 z (cm)
21 sphenix forward upgrade Sivers effect in Drell-Yan process Valence quark region at x 0.2 with 1 < η < 4 coverage Jet asymmetry Sivers effect or higher-twist effect Asymmetry inside of jets Collins effect twist 3 s = 200 GeV y=3.3 jets Fit of SIDIS SIDIS old jet h+x
22 August 23, J-PARC facility Materials and Life Science Experimental Facility Hadron Beam Facility Nuclear Transmutation 500 m Neutrino to Kamiokande Linac (330m) 3 GeV Synchrotron (25 Hz, 1MW) 50 GeV Synchrotron (0.75 MW) J-PARC = Japan Proton Accelerator Research Complex Joint Project between KEK and JAEA
23 J-PARC proposal/loi P04: measurement of high-mass dimuon production at the 50-GeV proton synchrotron deferred P12-LoI: study of parton distribution function of mesons via Drell-Yan process at J-PARC at high-p beamline P24: polarized proton acceleration at J-PARC no decision Possible stage-1? 30 GeV unpolarized proton beam & 5-20 GeV π/k beam + polarized target
24 Slide by W. Chang
25 Summary Fermilab SeaQuest experiment Unpolarized program Flavor asymmetry of sea-quark distribution Boer-Mulders distribution Cold Nuclear Matter (CNM) effect Physics run will start in late October (this month) Polarized Drell-Yan experiments Polarized Drell-Yan proposals of Fermilab program P1027 polarized beam experiment (stage-1 approval) P1039 polarized target experiment (stage-1 approval) PHENIX upgrade program at RHIC sphenix barrel and forward detector upgrade under discussion Possible J-PARC program Exclusive Drell-Yan measurement under development
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