9/19/20151 Nucleon Spin: Final Solution at the EIC Feng Yuan Lawrence Berkeley National Laboratory

Next Big Thing in QCD 9/19/20152

References: INT-Write-Up, “Gluons and the quark sea at high energies: distributions, polarization, tomography”, 500 pages, e-Print: arXiv: [nucl-th]. EIC-White Paper, “Electron-Ion Collider: Next QCD Frontier”,150 pages, e-Print: arXiv: [nucl-ex] 3

4 9/19/2015 QCD and Strong-Interactions QCD: Non-Abelian gauge theory  Building blocks: quarks (spin ½, m q, 3 colors; gluons: spin 1, massless, colors) Asymptotic freedom and confinement Clay Mathematics Institute Millennium Prize Problem Long distance:? Soft, non-perturbative Short distance hard, perturbative Nonperturbative scale  QCD ~1GeV ~1/Length

Understanding the nucleon 5 Solving QCD  Numeric simulation: Lattice QCD BMW, Science, 2008 LHPC, 2011

Understanding the nucleon 6 Experimental probes  Study the quark and gluon structure through low and high-energy scattering  Matrix elements of local operators (e.g., form factors) or operators on the light-cone (parton distributions)  High energy experiments  perturbative QCD, factorization, universality  Sum rules:  Momentum  Bjorken  Nucleon spin  …

Deep Inelastic Scattering 9/19/20157 FriedmanKendallTaylor Bjorken Scaling: Q 2  Infinity Feynman Parton Model: Point-like structure in Nucleon

In particular DIS (Virtual Photon Q>> ∧ QCD ) 9/19/20158 Leading Born Diagram Higher Order Corrections:  Gluon Momentum (divergence)  Collinear: xP, x-finite  Soft: xP+kt, x-small P

9 Factorization is essential to study nucleon structure Universality of the parton distributions  Predictive power of QCD Collins-Soper-Sterman 85, Bodwin 85, … Ji-Ma-Yuan 04, Dominguez-Xiao-Yuan 10,…

EIC Proposals in US 9/19/201510

Basics Inclusive DIS  Parton distributions Semi-inclusive DIS, measure additional hadron in final state  Kt-dependence Exclusive Processes, measure recoiled nucleon  Nucleon tomography Parity violating process 9/19/ Luminosity requirement

Big questions 9/19/201512

kt-dependence crucial to the saturation 13 QCD Phase structure of cold nuclei

Comprehensive study of small-x saturation at the EIC Inclusive observable Two-particle correlations 9/19/

Diffractions 9/19/201515

Hadronization in cold nuclei vs hot matter 9/19/201516

Intensity Frontier (EW Physics) 9/19/ √S = 140GeV, 200fb -1

189/19/2015 Ultimate goal of spin physics? Spin sum rule Quark spin, Best known Gluon spin, Start to know Orbital Angular Momentum of quarks and gluons, Little known Jaffe-Manohar, 90 Ji, 96

19 EMC experiment at CERN Polarized muon + p deep inelastic scattering,  Virtual photon can only couple to quarks with opposite spin, because of angular momentum conservation  Select q + (x) or q - (x) by changing the spin direction of the nucleon or the incident lepton  The polarized structure function measures the quark spin density

20 Summary of the polarized DIS data

EIC kinematics

23 Back to DIS With EIC

In particular

Quark spin x2 gluon spin

Where is the rest of spin Back to the angular momentum density Energy-momentum tensors in quark and gluon 9/19/201526

Spin sum rule Taking forward limit, 9/19/ Ji, 1996

28 Q2Q2 t A new type of parton “ distributions ” contains much more information Comprehensive program at JLab,HERMES,COMPASS and future EIC Quark OAM: L q Generalized Parton Distributions in hard exclusive processes: J q ( H + E) x dx = J q = 1/2  L z Mueller et al.,94;Ji,96; Radyushkin,96 (Ji 96)

Extract the GPDs The theoretical framework has been well established  Perturbative QCD corrections at NLO, some at NNLO 9/19/ Mueller, et al., J u, J d, J g

EIC kinematics coverage 9/19/201530

Further decomposition of J q Quark spin explicitly OAM, twist-three nature 9/19/2015 Ji, Xiong, Yuan, PRL109, (2012); PRD 13; Hatta, Yoshita, JHEP 2012; Liuti, et al.,

Related to the parton’s phase space Wigner Distributions 32 Phase space distribution: Projection onto p (x) to get the momentum (probability) density Quark orbital angular momentum Well defined in QCD: Ji, Xiong, Yuan, PRL, 2012; PRD, 2013 Lorce, Pasquini, Xiong, Yuan, PRD, 2012

Quark imaging from EIC 9/19/ Mueller, et al.,

Gluon Tomography toward small-x 9/19/201534

Nucleon tomography 9/19/201535

Transverse momentum dependent parton distribution Straightforward extension  Spin average, helicity, and transversity distributions P T -spin correlations  Nontrivial distributions, S T XP T  In quark model, depends on S- and P-wave interference 9/19/201536

9/19/ Quark Sivers function leads to an azimuthal asymmetric distribution of quark in the transverse plane Alex

Where can we learn TMDs Semi-inclusive hadron production in deep inelastic scattering (SIDIS) Drell-Yan lepton pair, photon pair productions in pp scattering Dijet correlation in DIS Relevant e+e- annihilation processes … 9/19/201538

39 9/19/2015 Novel Single Spin Asymmetries U: unpolarized beam T: transversely polarized target Semi-inclusive DIS Sivers: Collins:

EIC kinematics 9/19/201540

Precision of 3-D PDFs at EIC 9/19/201541

all order factorization 9/19/ Similar calculations for pp collisions: Zhu HX, et al., PRL110 (2013)

Conclusions: EIC Great opportunities in nuclear science Ultimate machine for nucleon spin physics Unique place to investigate gluon saturation Potential discovery in BSM physics 9/19/201543

TMDs in valence region Quark Sivers function leads to an azimuthal asymmetric distribution of quark in the transverse plane 9/19/ Alex

Current Research Focused on 45 Long. Momentum distributions Nucleon Spin 3D imaging Transverse-momentum-dependent and Generalized PDFs QCD: Factorization, Universality, Evolution, Lattice, …

Access the GPDs Deeply virtual Compton Scattering (DVCS) and deeply virtual exclusive meson production (DVEM) 9/19/ GPD In the Bjorken limit: Q 2 >>(-t), ∧ 2 QCD,M 2 Mueller, et al., hep-ph/ ,

Nucleon tomography and Orbital angular momentum Momentum P T Factorization: Ji-Ma-Yuan 2004 Coordinate B T

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