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E Entering the Electronic Age at RHIC: RHIC APS Division of Nuclear Physics Fall Meeting October 24, 2012 Christine A. Aidala University of Michigan.

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Presentation on theme: "E Entering the Electronic Age at RHIC: RHIC APS Division of Nuclear Physics Fall Meeting October 24, 2012 Christine A. Aidala University of Michigan."— Presentation transcript:

1 e Entering the Electronic Age at RHIC: RHIC APS Division of Nuclear Physics Fall Meeting October 24, 2012 Christine A. Aidala University of Michigan

2 Entering a new era: Quantitative QCD! QCD: Discovery and development –1973  ~2004 Since 1990s starting to consider detailed internal QCD dynamics that parts with traditional parton model ways of looking at hadrons—and perform phenomenological calculations using these new ideas/tools! –Various resummation techniques –Non-collinearity of partons with parent hadron –Non-linear evolution at small momentum fractions C. Aidala, DNP, October 24, 2012 pp   0  0 X M (GeV) Almeida, Sterman, Vogelsang PRD80, 074016 (2009) PRD80, 034031 (2009) Transversity Sivers Boer-Mulders Pretzelosity Worm gear Collinear Transverse-Momentum-Dependent Mulders & Tangerman, NPB 461, 197 (1996) 2

3 eRHIC A facility to bring this new era of quantitative QCD to maturity! Study in detail –“Simple” QCD bound states: Nucleons –Collections of QCD bound states: Nuclei –Hadronization C. Aidala, DNP, October 24, 2012 Collider energies: Focus on sea quarks and gluons 3

4 Lots of fundamental questions remain to be answered in QCD! At short distances the proton appears as a system of many quarks, antiquarks and gluons. How does this relate to the simple picture where the proton is made up of three quarks? What is the dynamical origin of sea quarks and gluons inside the proton? How is hadron structure influenced by chiral symmetry and its breaking? How does the proton spin originate at the microscopic level? C. Aidala, DNP, October 24, 2012 4

5 Fundamental questions... How are the sea quarks and gluons distributed in space and momentum inside the nucleon? How does the nuclear environment affect the distribution of quarks and gluons and their interactions in nuclei? Where does the saturation of gluon densities set in? How does confinement manifest itself in the structure of hadrons? How does a colored quark or gluon become a colorless object? C. Aidala, DNP, October 24, 2012 5  s ~1  s << 1

6 Why eRHIC? Electroweak probe –“Clean” processes to interpret (QED) –Measurement of scattered electron  full kinematic information on partonic scattering Collider mode  Higher energies –Quarks and gluons relevant d.o.f. –Perturbative QCD applicable –Heavier probes accessible (e.g. charm, bottom, W boson exchange) C. Aidala, DNP, October 24, 2012 6 A very flexible facility: wide range of beam species and energies

7 Accelerator capabilities Polarized beams of p, He 3 –Previously only fixed-target polarized DIS experiments! Beams of light  heavy ions –Previously only fixed-target e+A experiments! Luminosity 1000x that of HERA e+p collider C. Aidala, DNP, October 24, 2012 7

8 Accessing quarks and gluons through DIS Measure of resolution power Measure of inelasticity Measure of momentum fraction of struck quark Kinematics: Quark splits into gluon splits into quarks … Gluon splits into quarks higher √s increases resolution 10 -19 m 10 -16 m 8

9 Access the gluons in DIS via scaling violations: dF 2 /dlnQ 2 and linear DGLAP evolution in Q 2  G(x,Q 2 ) OR Via F L structure function OR Via dihadron production  See L. Zheng’s talk 10/27 OR Via diffractive scattering  See M. Lamont’s talk 10/25 C. Aidala, DNP, October 24, 2012 Accessing gluons with an electroweak probe Gluons dominate low-x wave function ! Gluons in fact dominate (not-so-)low-x wave function! 9

10 New opportunities for DIS with polarized beams Proton helicity structure C. Aidala, DNP, October 24, 2012 10 Current data vs. eRHIC phase space 4.6x10 -3 (COMPASS) RHIC p+p data: constrain Δg(x) for ~ 0.05 < x < 0.2 X  2 decades Q 2 2 decades 5x100 GeV eRHIC Stage 1 20x250 GeV eRHIC Stage 2

11 Pinning down sea quark + gluon helicity distribution functional forms C. Aidala, DNP, October 24, 2012 11 Plots include only eRHIC stage-1 data (5 GeV electron beam) Semi-inclusive DIS data (measure produced hadron in addition to scattered electron) provide flavor separation of sea quarks

12 Spin-momentum correlations in QCD: Transverse-momentum-dependent (TMD) distribution and fragmentation functions Clean access to partonic kinematics in (semi- inclusive) DIS –Semi-inclusive DIS: Measure produced hadron in addition to scattered electron –More info than inclusive DIS C. Aidala, DNP, October 24, 2012 12 Can isolate the various TMD pdfs and FFs via measured angular dependences

13 Example: Sivers function C. Aidala, DNP, October 24, 2012 13 See talk by T. Burton, 10/27 High luminosity  measure transverse single-spin asymmetry vs. x differentially in Q 2, p T and z. Correlation between quarks’ transverse momentum and proton’s transverse spin Quark densities in transverse momentum plane for a proton polarized in the +y direction. Up and down quarks orbiting in opposite directions??

14 Perform spatial imaging via exclusive processes  Detect all final-state particles  Nucleon doesn’t break up Measure cross sections vs. four- momentum transferred to struck nucleon: Mandelstam t Goal: Cover wide range in t. Fourier transform  impact- parameter-space profiles Spatial imaging of the nucleon Obtain b profile from slope vs. t. C. Aidala, DNP, October 24, 2012 14 See talk by T. Burton, 10/27

15 Nuclei: Simple superpositions of nucleons? C. Aidala, DNP, October 24, 2012 No!! Rich and intriguing differences compared to free nucleons, which vary with the linear momentum fraction probed (and likely transverse momentum, impact parameter,...). Understanding the nucleon in terms of the quark and gluon d.o.f. of QCD does NOT allow us to understand nuclei in terms of the colored constituents inside them! 15

16 Lots of ground to cover in e+A! What is the role of strong gluon fields, parton saturation effects, and collective gluon excitations in nuclei? Can we experimentally find evidence of nonlinear QCD dynamics in high-energy scattering off nuclei? What are the momentum and spatial distributions of gluons and sea quarks in nuclei? Are there strong quark and gluon density fluctuations inside a large nucleus? How does the nucleus respond to the propagation of a color charge through it? C. Aidala, DNP, October 24, 2012 16

17 Nuclear modification of partonic structure C. Aidala, DNP, October 24, 2012 17 What’s the behavior of low-x gluons in nuclei?? Large extrapolation uncertainty on global fit to existing fixed-target data Greatly reduced with EIC data!

18 C. Aidala, DNP, October 24, 2012 Bremsstrahlung ~  s ln(1/x) x = P parton /P nucleon small x Recombination ~  s  Gluon saturation  s ~1  s << 1   At small x linear evolution gives strongly rising g(x)  violation of Froissart unitary bound  BK/JIMWLK non-linear evolution includes recombination effects  saturation  Dynamically generated scale Saturation Scale: Q 2 s (x)  Increases with energy or decreasing x  Scale with Q 2 /Q 2 s (x) instead of x and Q 2 separately 18

19 Gluon saturation Nuclear enhancement of saturation scale: can reach this non-linear QCD regime at higher x (lower energies) than in e+p Multiple handles to study saturation regime, e.g. –Dihadron correlations – See L. Zheng’s talk, 10/27 –Diffractive scattering Inclusive diffractive structure function for nuclei Exclusive diffractive production of vector mesons C. Aidala, DNP, October 24, 2012 19

20 Impact-parameter-dependent nuclear gluon density via exclusive vector meson production Just like in optics—the positions of the diffractive minima are related to the size of the obstacle Low t: Coherent diffraction dominates – gluon density High t: Incoherent diffraction dominates – gluon correlations C. Aidala, DNP, October 24, 2012 20 These exclusive measurements sensitive to saturation effects!

21 Hadronization at eRHIC C. Aidala, DNP, October 24, 2012 21 Use nuclei as femtometer-scale detectors of the hadronization process! Wide range of scattered parton energy; small to large nuclei –Move hadronization inside/outside nucleus –Distinguish energy loss and attenuation Comprehensive studies of hadronization as well as of propagation of color charges through nuclei possible at eRHIC!

22 eRHIC accelerator C. Aidala, DNP, October 24, 2012 22 Initial E e ~ 5 GeV. Install additional RF cavities over time to reach E e = 30 GeV. All magnets installed from day one E e ~5-20 GeV (30 GeV w/ reduced lumi) E p 50-250 GeV E A up to 100 GeV/n

23 Detector concepts Detector will need to measure Inclusive processes –Detect scattered electron with high precision Semi-inclusive processes –Detect at least one final-state hadron in addition to scattered electron Exclusive processes –Detect all final-state particles in the reaction C. Aidala, DNP, October 24, 2012 23 Large detector acceptance: |  < ~5 Low radiation length critical  low electron energies Precise vertex reconstruction  separate b and c DIRC/RICH  , K, p hadron ID Forward detectors to tag proton in exclusive reactions Latest call for Electron-Ion Collider detector R&D proposals: https://wiki.bnl.gov/conferences/index.php/EIC_R%25D

24 We’ve recently moved beyond the discovery and development phase of QCD into a new era of quantitative QCD! eRHIC, capable of colliding polarized electrons with a variety of unpolarized nuclear species as well as polarized protons and polarized light nuclei over center-of-mass energies from ~30 to ~175 GeV, could provide experimental data to bring this new era to maturity over the upcoming decades! Summary C. Aidala, DNP, October 24, 2012 24 Electron-Ion Collider White Paper recently released! http://www.bnl.gov/rhic/eicrev/ch/ch-files/c1-c6.pdf

25 C. Aidala, DNP, October 24, 2012 Additional Material 25

26 Key measurements of the nucleon C. Aidala, DNP, October 24, 2012 26 Spin and flavor 3-D structure: transverse momentum dependence 3-D structure: spatial imaging

27 Key measurements of nuclei C. Aidala, DNP, October 24, 2012 27 High gluon densities Non-saturation regime

28 eRHIC e+p luminosities C. Aidala, DNP, October 24, 2012 28

29 C. Aidala, DNP, October 24, 2012 3D quantum phase-space tomography of the nucleon 3D picture in coordinate space: generalized parton distributions Polarized p d-quark u-quark Polarized p TMDs GPDs Wigner Distribution W(x,r,k t ) 3D picture in momentum space: transverse-momentum- dependent distributions 29

30 Probing gluon Sivers function via D mesons C. Aidala, DNP, October 24, 2012 30

31 C. Aidala, DNP, October 24, 2012 Spatial imaging: Gluon vs quark distributions in impact parameter space Do singlet quarks and gluons have the same transverse distribution? Hints from HERA: Area (q+q) > Area g - Singlet quark size e.g. from deeply virtual Compton scattering Gluon size e.g. from J/  electroproduction 31 Deeply Virtual Compton Scattering

32 DVCS kinematic coverage C. Aidala, DNP, October 24, 2012 32

33 C. Aidala, DNP, October 24, 2012 Q s : A scale that binds them all Freund et al., hep-ph/0210139 Nuclear shadowing Geometrical scaling Is the wave function of hadrons and nuclei universal at low x? proton  5 nuclei 33

34 C. Aidala, DNP, October 24, 2012 34

35 C. Aidala, DNP, October 24, 2012 Exclusive processes: Collider energies 35

36 Dihadron correlations in e+A scattering: Sensitive to saturation C. Aidala, DNP, October 24, 2012 36

37 Hadronization and energy loss nDIS: – Clean measurement in ‘cold’ nuclear matter – Suppression of high-p T hadrons analogous but weaker than at RHIC Fundamental question: When do coloured partons get neutralized? Parton energy loss vs. (pre)hadron absorption Energy transfer in lab rest frame EIC: 10-1600 GeV 2 HERMES: 2-25 GeV 2 EIC can measure heavy flavor energy loss C. Aidala, DNP, October 24, 2012 37

38 Hadronization and energy loss Difference in z dependence of pion and D FFs Striking difference in multiplicity ratio (e+Pb/e+p) for D vs. pion production—slopes sensitive to transport coefficients C. Aidala, DNP, October 24, 2012 38

39 no y cut y > 0.1 Q 2 > 1 GeV 2 20×250HERA Charged-current cross section C. Aidala, DNP, October 24, 2012 39

40 Measuring sin 2  W at the EIC C. Aidala, DNP, October 24, 2012 40 √s = 140 GeV 200 fb -1

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