1. Electric Dipole Moment of the Deuteron Experiment: EDM Violates T-Symmetry: Connected to CP-Violation and the Matter-Antimatter Asymmetry of the Universe. EDMs are Excellent Probes of Physics Beyond the SM. 10/14/2003 Y.k. Semertzidis

2. EDM Collaboration M. Aoki 13, M. Auzinsh 9, V. Balakin 2, A. Bazhan 2, G.W. Bennett 4, R.M. Carey 3, P. Cushman 10, P.T. Debevec 7, A. Dudnikov 2, F.J.M. Farley 15, D.W. Hertzog 7, M. Iwasaki 14, K. Jungmann 5, D. Kawall 15, B. Khazin 2, I.B. Khriplovich 2, B. Kirk 4, Y. Kuno 13, D.M. Lazarus 4, L.B. Leipuner 4, V. Logashenko 2,3, K.R. Lynch 3, W.J. Marciano 4, R. McNabb 10, W. Meng 4, J.P. Miller 3, *, W.M. Morse 4, C.J.G. Onderwater 7, Y.F. Orlov 6, C.S. Ozben 7, R. Prigl 4, S. Redin 2, S. Rescia 4, B.L. Roberts 3, Y.K. Semertzidis 4, *, N. Shafer-Ray 11, A. Silenko 1, E.J. Stephenson 8, K. Yoshimura 12 1. Belarusian State University, Belarus; 2. BINP, Novosibirsk; 3. Boston University; 4. Brookhaven National Laboratory; 5. Kernfysisch Versneller Instituut, Groningen; 6. Newman Laboratory, Cornell University, Ithaca; 7. University of Illinois, at Urbana-Champaign; 8. Indiana University; 9. University of Latvia; 10. University of Minnesota; 11. University of Oklahoma; 12. KEK, Japan; 13. Osaka University, Japan; 14. RIKEN, Japan; 15. Department of Physics, Yale University, New Haven. * Spokesperson

3. Radial E-field to Cancel the g-2 Precession in a Storage Ring: Radial E-Field: The method works well for particles with small anomalous magnetic moment a, like deuterons (a = -0.143), etc.

4. Deuteron Statistical Error @ BNL:  p : 3s. Polarization Lifetime (Coherence Time) A : 0.3. The left/right asymmetry observed by the polarimeter P : 0.55. The beam polarization N c : 10 11 d/cycle. The total number of stored particles per cycle T Tot : 10 7 s. Total running time f : 0.1. Useful event rate fraction E R : 3.5MV/m. Radial electric field

5. Deuteron EDM at 10 -27 e  cm: It Improves the T-odd Nuclear Forces Limits from 199 Hg by a Factor of 100. (Sushkov, Flambaum, Khriplovich Sov. Phys. JETP, 60, p. 873 (1984) and Khriplovich and Korkin, Nucl. Phys. A665, p. 365 (2000)). It Improves the Current Proton EDM Limit by a Factor of ~100,000 and that of the Neutron by a Factor of ~100.

6. What’s Needed: An Optimized Ring for Measuring the EDM of the Deuteron: R~30m, B~0.13T, E~3.5MV/m, 8  2m Long Straight Sections for Polarimeters. Cost:~$20M (Includes G&A plus 25% Contingency) 10 11 Polarized Deuterons/cycle of 1GeV/c Momentum. Deuteron Polarimeters. Well Matched with BNL Expertise and Capabilities…

7. Proposal Early Next Year… Sensitive EDM Experiments will bring the Next Breakthrough in Elementary Particle Physics; BNL Can & Should Play a Prominent Role in this Field. We are close to finishing working on the systematics, aiming for a

8. EDM of Hadrons: Neutron: n |d n | < 6.0  10 -26 e·cm (90%CL) PRL 82, 904 (1999) Diamagnetic Atoms, 199 Hg: |d( 199 Hg)| < 2.1  10 -28 e·cm (95%CL) PRL 86, 2505 (2001)

9. Predictions in Specific Models The predicted value for the electron is 10 times less than the current experimental limit. 50  effect at 10 -24 e  cm Exp. Sensitivity!

10. Muon EDM Experiment: (http://www.bnl.gov/edm) Need NP 2 =10 16 for 10 -24 e  cm. Muon EDM LOI to J-PARC, <one year of running. Systematics much less than 10 -24 e  cm Beam Power at J-PARC 8 times of AGS We have received strong encouragement from the J-PARC Project Manager to Submit a Proposal

11. x y z  Tot dd aa  x y z dd aa  Canceling the g-2 precession…