1. POETIC 2012 Indiana University R. D. McKeown 12 GeV CEBAF

2. 2 W p u (x,k T,r ) Wigner distributions d2kTd2kT PDFs f 1 u (x),.. h 1 u (x)‏ d3rd3r TMD PDFs f 1 u (x,k T ),.. h 1 u (x,k T )‏ 3D imaging 6D Dist. Form Factors G E (Q 2 ), G M (Q 2 )‏ d2rTd2rT dx & Fourier Transformation 1D Unified View of Nucleon Structure GPDs/IPDs d 2 k T dr z

3. 3 t hard vertices A =           = Unpolarized beam, transverse target:  UT ~ sin  {k(F 2 H – F 1 E ) }d  E(  t)  LU ~ sin  {F 1 H + ξ(F 1 +F 2 ) H +kF 2 E }d  ~ Polarized beam, unpolarized target: H( ,t) ξ=x B /(2-x B ) Unpolarized beam, longitudinal target:  UL ~ sin  {F 1 H +ξ(F 1 +F 2 )( H +ξ/(1+ξ) E) }d  ~ H( ,t) ~ Cleanest process: Deeply Virtual Compton Scattering

4. 4 DVCS beam asymmetry at 12 GeV CLAS12 ep ep  High luminosity and large acceptance allows wide coverage in Q 2 < 8 GeV 2, x B < 0.65, and t< 1.5GeV 2 sinφ moment of A LU

5. 5 SIDIS Electroproduction of Pions Separate Sivers and Collins effects Sivers angle, effect in distribution function: (  h -  s ) Collins angle, effect in fragmentation function: (  h +  s ) Scattering Plane target angle hadron angle Previous data from HERMES,COMPASS New landscape of TMD distributions Access to orbital angular momentum

6. 6 SoLID Transversity Projected Data Total 1400 bins in x, Q 2, P T and z for 11/8.8 GeV beam. z ranges from 0.3 ~ 0.7, only one z and Q 2 bin of 11/8.8 GeV is shown here. π + projections are shown, similar to the π -.

7. 7 Quark Angular Momentum 7 → Access to quark orbital angular momentum

8. 8 Parity Violating Electron Scattering 8

9. 9 12 GeV With 12 GeV we study mostly the valence quark component An EIC aims to study gluon dominated matter. Into the “sea”: EIC mEIC EIC

10. 10

11. 11 TMD studies at EIC 10 fb -1 @ each s (from EIC White Paper)

12. 12 Extending Sivers Tomography A. Prokudin

13. 13 Longitudinal Spin -  G 10 fb -1 – Stage 1 (from EIC White Paper)

14. 14 Gluon Tomography DV J/  Production (from EIC White Paper)

15. 15 Precision Tests of the Standard Model 200 fb -1

16. 16 MEIC Design Report Web posting imminent Stable design for 3 years

17. 17 Medium Energy EIC@JLab JLab Concept Initial configuration (MEIC): 3-11 GeV on 20-100 GeV ep/eA collider fully-polarized, longitudinal and transverse luminosity: up to few x 10 34 e-nucleons cm -2 s -1 Upgradable to higher energies (250 GeV protons) Pre-booster Ion source Transfer beam line Medium energy IP Electron collider ring (3 to 11 GeV) Injector 12 GeV CEBAF SRF linac Warm large booster (up to 20 GeV) Cold ion collider ring (up to 100 GeV)

18. 18 solenoid electron FFQs 50 mrad 0 mrad ion dipole w/ detectors ions electrons IP ion FFQs 2+3 m 2 m Detect particles with angles below 0.5 o beyond ion FFQs and in arcs. Need 4 m machine element free region detectors Central detector Detect particles with angles down to 0.5 o before ion FFQs. Need 1-2 Tm dipole. EM Calorimeter Hadron Calorimeter Muon Detector EM Calorimeter Solenoid yoke + Muon Detector TOF HTCC RICH RICH or DIRC/LTCC Tracking 2m 3m 2m 4-5m Solenoid yoke + Hadronic Calorimeter Very-forward detector Large dipole bend @ 20 meter from IP (to correct the 50 mr ion horizontal crossing angle) allows for very-small angle detection (<0.3 o ). Need 20 m machine element free region Full MEIC: Full Acceptance Detector 7 meters Three-stage detection

19. 19 My View Going Forward There has been excellent progress on developing the EIC science case over the last 2 years, and even more since the INT program. There have been important contributions from both the BNL and JLab communities. I continue to believe that it is essential that these two communities work together to realize the recommendation of an EIC by the broader nuclear physics community. Completing the White Paper is a crucial next step in this process. Many thanks to the WP writers/editors.