490 likes | 572 Views
Nucleon Spin: Final Solution at the EIC. Feng Yuan Lawrence Berkeley National Laboratory. Next Big Thing in QCD. References:. INT-Write-Up, “ Gluons and the quark sea at high energies: distributions, polarization, tomography ” , 500 pages, e-Print: arXiv:1108.1713 [nucl-th].
E N D
Nucleon Spin: Final Solution at the EIC Feng Yuan Lawrence Berkeley National Laboratory
References: • INT-Write-Up, “Gluons and the quark sea at high energies: distributions, polarization, tomography”, 500 pages, e-Print: arXiv:1108.1713 [nucl-th]. • EIC-White Paper, “Electron-Ion Collider: Next QCD Frontier”,150 pages, e-Print: arXiv:1212.1701 [nucl-ex]
Clay Mathematics Institute Millennium Prize Problem QCD and Strong-Interactions • QCD: Non-Abelian gauge theory • Building blocks: quarks (spin ½, mq, 3 colors; gluons: spin 1, massless, 32-1 colors) • Asymptotic freedom and confinement Short distance hard, perturbative Long distance:? Soft, non-perturbative ~1/Length Nonperturbative scale QCD~1GeV
Understanding the nucleon • Solving QCD • Numeric simulation: Lattice QCD BMW, Science, 2008 LHPC, 2011
Understanding the nucleon • 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 Friedman Kendall Taylor Bjorken Scaling: Q2Infinity Feynman Parton Model: Point-like structure in Nucleon
In particular • DIS (Virtual Photon Q>>∧QCD) Leading Born Diagram P • Higher Order Corrections: • Gluon Momentum (divergence) • Collinear: xP, x-finite • Soft: xP+kt, x-small
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,…
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 Luminosity requirement
QCD Phase structure of cold nuclei • kt-dependence crucial to the saturation
Comprehensive study of small-x saturation at the EIC Inclusive observable Two-particle correlations xiao@EIC-Whitepaper
Intensity Frontier (EW Physics) √S = 140GeV, 200fb-1
Ultimate goal of spin physics? • Spin sum rule Jaffe-Manohar, 90 Ji, 96 Quark spin, Best known Gluon spin, Start to know Orbital Angular Momentum of quarks and gluons, Little known
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
Back to DIS With EIC
gluon spin Quark spin x2
Where is the rest of spin • Back to the angular momentum density • Energy-momentum tensors in quark and gluon
Spin sum rule Ji, 1996 • Taking forward limit,
Q2 t ( H + E) x dx =Jq Quark OAM: Lq = 1/2 DS+ Lz (Ji 96) Generalized Parton Distributions in hard exclusive processes: • A new type of parton “distributions” contains much more information • Comprehensive program at JLab,HERMES,COMPASS and future EIC Mueller et al.,94;Ji,96; Radyushkin,96
Extract the GPDs • The theoretical framework has been well established • Perturbative QCD corrections at NLO, some at NNLO Mueller, et al., 1310.5394 Ju, Jd, Jg
Further decomposition of Jq • Quark spin explicitly • OAM, twist-three nature Ji, Xiong, Yuan, PRL109, 152005 (2012); PRD 13; Hatta, Yoshita, JHEP 2012; Liuti, et al., 1310.5157
Related to the parton’s phase space Wigner Distributions 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 Mueller, et al., 1304.0077
Transverse momentum dependent parton distribution • Straightforward extension • Spin average, helicity, and transversity distributions • PT-spin correlations • Nontrivial distributions, STXPT • In quark model, depends on S- and P-wave interference
Alex Prokudin @EIC-Whitepaper Quark Sivers function leads to an azimuthal asymmetric distribution of quark in the transverse plane
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 • …
Semi-inclusive DIS • Novel Single Spin Asymmetries Collins: U: unpolarized beam T: transversely polarized target Sivers:
all order factorization Similar calculations for pp collisions: Zhu HX, et al., PRL110 (2013) 082001
Conclusions: EIC • Great opportunities in nuclear science • Ultimate machine for nucleon spin physics • Unique place to investigate gluon saturation • Potential discovery in BSM physics
TMDs in valence region Alex Prokudin @EIC-Whitepaper Quark Sivers function leads to an azimuthal asymmetric distribution of quark in the transverse plane
Current Research Focused on QCD: Factorization, Universality, Evolution, Lattice, … Nucleon Spin Long. Momentum distributions 3D imaging Transverse-momentum-dependent and Generalized PDFs
Access the GPDs • Deeply virtual Compton Scattering (DVCS) and deeply virtual exclusive meson production (DVEM) GPD In the Bjorken limit: Q2>>(-t),∧2QCD,M2 Mueller, et al., hep-ph/0112108, 1310.5394
Nucleon tomography and Orbital angular momentum Coordinate BT Momentum PT Factorization: Ji-Ma-Yuan 2004