1. Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Stony Brook, Dec 8 2007 Physics Topics Working Group Organisation Status of Simulations Plans for the Future

2. Physics Topics inclusive physics unpolarised structure funcions polarised struture functions electroweak physics tests of standard model electroweak structur functions semi-inclusive physics current quark fragmentation and flavour separation target fragmentation and correlation between current and target fragmentation polarised gluon distribution  G charm production jets

3. Physics Topics azimuthal asymmetries Transverse Momentum Dependent Parton Distributions Sivers and Collins functions Orbital momentum ? exclusive processes and diffraction DVCS Meson production 3 dimensional image of the proton orbital momentum ? Photoproduction

4. The Gluon Contribution to the Nucleon Spin Antje Bruell, Jlab EIC meeting, MIT, April 7 2007 Introduction  G from scaling violations of g 1 (x,Q 2 ) The Bjorken Sum Rule  G from charm production

5. The Gluon Contribution to the Nucleon Spin Antje Bruell, Jlab EIC meeting, MIT, April 7 2007 Introduction  G from scaling violations of g 1 (x,Q 2 ) The Bjorken Sum Rule  G from charm production

6. The Gluon Contribution to the Nucleon Spin Antje Bruell, Jlab EIC meeting, MIT, April 7 2007 Introduction  G from scaling violations of g 1 (x,Q 2 ) The Bjorken Sum Rule  G from charm production

7. The Gluon Contribution to the Nucleon Spin Antje Bruell, Jlab EIC meeting, MIT, April 7 2007 Introduction  G from scaling violations of g 1 (x,Q 2 ) The Bjorken Sum Rule  G from charm production

8. World Data on g 1 p < 2 orders of magnitude, precision !!! EIC Data on g 1 p Sufficient coverage in x and Q 2 to detrmine  G

9.  G from scaling violations of g 1

10. g 1 and the Bjorken Sum Rule

11. Bjorken Sum Rule 3-4% precision at various values of Q 2 Needs: O(1%) Ion Polarimetry!!! excellent determination of  s (Q 2 ) Sub-1% statistical precision at ELIC (averaged over all Q 2 )

12. RHIC-Spin region Precisely image the sea quarks Spin-Flavor Decomposition of the Light Quark Sea | p = + + + … > u u d u u u u d u u d d d Many models predict  u > 0,  d < 0

13. c c D mesons Polarized gluon distribution via charm production LO QCD: asymmetry in D production directly proportional to  G/G very clean process !

14. Polarized gluon distribution via charm production Precise determination of  G/G for 0.003 < x g < 0.4 at common Q 2 of 10 GeV 2 however  RHIC SPIN

15. If: We can measure the scattered electron even at angles close to 0 0 (determination of photon kinematics) We can separate the primary and secondary vertex down to about 100  m We understand the fragmentation of charm quarks (  ) We can control the contributions of resolved photons We can calculate higher order QCD corrections (  ) Polarized gluon distribution via charm production Precise determination of  G/G for 0.003 < x g < 0.4 at common Q 2 of 10 GeV 2

16. Need to measure the scattered electron at angles close to 0 0  how ? Need to separate the primary and secondary vertex down to about 100  m  how to determine the primary vertex ? For charm decay products need to instrument only  15- 20 0 around proton direction Simple set of silicon disks might be sufficient for vertex detection Momenta of decay products between 1.5 and 10(15) GeV charm production: detector consequences

17. ELIC Vanish like 1/p T (Yuan) Correlation between Transverse Spin and Momentum of Quarks in Unpolarized Target All Projected Data Perturbatively Calculable at Large p T

18. The Gluon Contribution to the Nucleon Spin Antje Bruell, Jlab EIC meeting, MIT, April 7 2007 Introduction  G from scaling violations of g 1 (x,Q 2 ) The Bjorken Sum Rule  G from charm production

19. The Gluon Contribution to the Nucleon Spin Antje Bruell, Jlab EIC meeting, MIT, April 7 2007 Introduction  G from scaling violations of g 1 (x,Q 2 ) The Bjorken Sum Rule  G from charm production

20. The Gluon Contribution to the Nucleon Spin Antje Bruell, Jlab EIC meeting, MIT, April 7 2007 Introduction  G from scaling violations of g 1 (x,Q 2 ) The Bjorken Sum Rule  G from charm production

21. Summary and Next Steps goals: realistic estimates for key processes consequencs for detector design for all key processes status: realistic estimates for very few processes hardly any idea about detector constrains simulation of some more processes just started several interested people identified next steps: continue in identification of people interested/capable to do some real work start working group meetings (around collaboration meetings)