Drell-Yan experiments at Fermilab/RHIC/J-PARC. QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN)

Similar documents
Sea-quark spin/flavor with Drell-Yan experiments. INT Workshop Orbital Angular Momentum in QCD February 15, 2012 Yuji Goto (RIKEN)

SSA Measurements with Primary Beam at J-PARC

GPDs and TMDs at Electron-Ion Collider. Workshop on hadron tomography at J-PARC and KEKB January 6 th, 2017 KEK, Tsukuba, Japan Yuji Goto (RIKEN)

Nucleon Spin Structure: Overview

Polarized Drell-Yan Experiment at J-PARC. J-PARC Meeting for Spin and Hadron Physics Nishina Hall at RIKEN April 7 th, 2008 Yuji Goto (RIKEN/RBRC)

Probing nucleon structure by using a polarized proton beam

Quarkonium Production at J-PARC

Studies on transverse spin properties of nucleons at PHENIX

COMPASS Drell-Yan. Michela Chiosso, University of Torino and INFN. TMD ECT* Workshop April 2016

Contributions to our Understanding of TMDs from Polarized Proton Collisions at STAR

Experimental Program of the Future COMPASS-II Experiment at CERN

Study of the hadron structure using the polarised Drell-Yan process at COMPASS

Central Questions in Nucleon Structure

Electron-Ion Collider for Nuclear and Particle Physics. Hugh Montgomery Jefferson Lab

Measurements with Polarized Hadrons

COMPASS Measurements of Asymmetry Amplitudes in the Drell-Yan Process Observed from Scattering Pions off a Transversely Polarized Proton Target

Transverse SSA Measured at RHIC

The Jlab 12 GeV Upgrade

Nucleon Spin Structure Longitudinal Spin of the Proton. HUGS Summer School Jefferson National Laboratory June 2, 2011 Lecture 5

Helicity: Experimental Status. Matthias Grosse Perdekamp, University of Illinois

Possible relations between GPDs and TMDs

Recent transverse spin results from STAR

TMDs and the Drell-Yan process

MEIC Central Detector Zhiwen Zhao for JLab MEIC Study Group

Measuring the gluon Sivers function at a future Electron-Ion Collider

Transverse Momentum Dependent Parton Distributions

Fundamental Open Questions in Spin Physics

Drell-Yan Experiment with J-PARC Polarized Proton Beam. IWHSS08 in Torino April 2 nd, 2008 Yuji Goto (RIKEN/RBRC)

QCD Collinear Factorization for Single Transverse Spin Asymmetries

Spin Structure of the Nucleon: quark spin dependence

Hall A/C collaboration Meeting June Xuefei Yan Duke University E Collaboration Hall A collaboration

Electron-Ion Collider Taking us to the next QCD Frontier

Meson Structure with Dilepton Production

erhic: Science and Perspective

Transverse Spin Structure with muon beam and Drell-Yan measurements at COMPASS

Generalized Parton Distributions Program at COMPASS. QCD Evolution 2015

Summary of Workshop on Spin of Nucleons from Low to High Energy Scales

a medium energy collider taking nucleon structure beyond the valence region

TMDs at Electron Ion Collider Alexei Prokudin

Recent Development in Proton Spin Physics

Lepton Angular Distributions in Drell-Yan Process

First results of W ± boson production in high-energy polarized p+p collisions at RHIC at BNL

Studying Evolution with Jets at STAR. Renee Fatemi University of Kentucky May 28 th, 2015

Heavy-ion collisions in a fixed target mode at the LHC beams

Experimental investigation of the nucleon transverse structure

Transverse Spin Effects and k T -dependent Functions

Flavor Asymmetry of the Nucleon Sea and W-Boson Production*

Measuring the gluon Sivers function at a future Electron-Ion Collider

Scale dependence of Twist-3 correlation functions

High-energy hadron physics at J-PARC

Nucleon spin and parton distribution functions

Transversity experiment update

Longitudinal Double Spin Asymmetry in Inclusive Jet Production at STAR

QCD Factorization and Transverse Single-Spin Asymmetry in ep collisions

Strong interaction physics with an Electron Ion Collider

Study of transverse momentum dependent distributions from polarised Drell-Yan at COMPASS

HERMES at HERA: Quark-Gluon Spin Structure of the Nucleon

The Detector Design of the Jefferson Lab EIC

Selected results and future prospects of the high-energy polarized p+p program at RHIC at BNL

High Energy Physics. Lecture 9. Deep Inelastic Scattering Scaling Violation. HEP Lecture 9 1

Polarised Drell-Yan Process in the COMPASS Experiment

PoS(DIS2018)216. W Measurement at PHENIX. Chong Kim

Two Photon Exchange in Inclusive and Semi Inclusive DIS

An Electron Ion Collider in China Xurong Chen

Measurements of unpolarized azimuthal asymmetries. in SIDIS at COMPASS

Electron-Ion Collider for Nuclear and Particle Physics. Hugh Montgomery Jefferson Lab

Tagging with Roman Pots at RHIC. Proton tagging at STAR

Flavor Decomposition of Nucleon Spin via polarized SIDIS: JLab 12 GeV and EIC. Andrew Puckett Los Alamos National Laboratory INT 09/24/2010

The STAR Transverse Spin Program

Nucleon Spin. Tyler Corbett

Single Spin Asymmetries on proton at COMPASS

Particle Physics with Electronic Detectors

THE NUCLEUS AS A QCD LABORATORY: HADRONIZATION, 3D TOMOGRAPHY, AND MORE

The Physics Program of CLAS12

E1039 Polarized SeaQuest

Highlights from RHIC Spin Program

JAMboree. Theory Center Jamboree Jefferson Lab, Dec 13, Pedro Jimenez Delgado

Christine Aidala Columbia University Transversity 2004, Trento June 14, 2004

Present and Future Exploration of the Nucleon Spin and Structure at COMPASS

Anomalous Drell-Yan asymmetry from hadronic or QCD vacuum effects

Polarizing Helium-3 for down quark spin enrichment. Nigel Buttimore

Exciting opportunities at JLab GeV!

Installed and commissioned during run 4 To be commissioned Installed/commissioned in run /10/2005 Raimondo Bertini

Distribution Functions

The Electron-Ion Collider: Exploring the science of Nuclear Femtography

STAR upgrade program and future physics

Phenomenological applications of QCD threshold resummation

PANDA. antiproton Annihilation at DArmstadt

Monte-Carlo simulations for Drell-Yan in COMPASS

The future COMPASS-II Drell-Yan program

Prospects for Detecting Local Parity Violating Effects in Quark Fragmentation at. and

Spin physics at Electron-Ion Collider

Lessons from Lepton-Nucleon and Lepton-Nuclei Interactions Probing the structure of the atomic nucleus

Toward the QCD Theory for SSA

The Jefferson Lab 12 GeV Program

The RHIC SPIN Program

Direct measurement of the W boson production charge asymmetry at CDF

Factorization, Evolution and Soft factors

Polarized deuterium physics with EIC C. Weiss (JLab), Tensor Polarized Solid Target Workshop, JLab, 11 Mar 14

Transcription:

Drell-Yan experiments at Fermilab/RHIC/J-PARC QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN)

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

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

Flavor asymmetry of sea-quark distribution Fermilab-E866/NuSea experiment E beam = 800 GeV (from Tevatron) x = 0.01 0.35 (valence region) σ pd ~ 1 2 d ( x + 2) 1 u ( x ) pp 2σ 2 with CTEQ5M 1 0 0.35 0.015 dx[ d ( x) u ( x)] = 0.0803 ± 0.011 dx[ d ( x) u ( x)] = 0.118 ± 0.012

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

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

Flavor asymmetry of sea-quark distribution Fermilab-E906/SeaQuest experiment E beam = 120 GeV (from Main Injector) x = 0.1 0.45 Blue band: MSTW function refit error band with E866 data Yellow band: error band with E866 data + E906 expected statistics

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

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

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) 082301 Phys. Rev. Lett. 102 (2009) 182001 Error profile for SeaQuest statistics

SeaQuest commissioning run February 22 nd April 30 th, 2012 120 GeV/c proton beam, 19 ns interval (53 MHz) Beam intensity: 1.0 10 12 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)

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, 2013 2 year data accumulation (2013-2015) for 1.0 10 19 protons on target Beam intensity: 1.0 10 13 protons/spill (5s spill at 1 minute interval)

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

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

Polarized Drell-Yan experiment P1027 Polarized beam experiment May 18 th, 2012 proposal submitted November 14 th, 2012 stage-1 approval

Polarized Drell-Yan experiment P1027 Clean measurement of sign and shape of Sivers distributions to compare DIS and Drell-Yan 3.2 10 18 POT Red curve: prediction from SIDIS data (HERMES & COMPASS)

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 FY2013-2016

RHIC

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 2018-2019 Completion and experiment in 2021-2022 ephenix at erhic Transition to erhic in 2023-2024 Commissioning and experiment start in 2025

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)

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

August 23, 2010 22 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

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

Slide by W. Chang

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