Electric Dipole Moments A Window for New Physics
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1 Mitglied der Helmholtz-Gemeinschaft EPS Conference on High Energy Physics, July 2015, Vienna Electric Dipole Moments A Window for New Physics July 2015 Hans Ströher (Forschungszentrum Jülich)
2 New physics: empirical evidence (n-oscillations, dark matter, baryon asymmetry) doesn t a priori point to a specific mass scale Direct searches ( energy frontier ) Indirect searches ( precision frontier ) Precision observables that vanish (or are suppressed) by symmetry in the SM allow for new physics searches with indirect reach in both Energy scale Strength of coupling Example: new CP-odd sources EDMs Required for baryogenesis (Sakharov conditions) Strong CP problem (suppression of q QCD ) 25. Juli 2015 Institut für Kernphysik (IKP) Folie 2
3 Permanent Electric Dipole Moments (EDM) of nondegenerate fundamental systems (particles): A vector (d), connecting the centroids of positive and negative charge distributions, in the direction of the spin vector (µ). 25. Juli 2015 Institut für Kernphysik (IKP) Folie 3
4 Permanent Electric Dipole Moments (EDM) of nondegenerate fundamental systems (particles): Spin EDM + T Original illustration by: physicsworld.com violate P- and T-, and (via CPT) also CP-symmetry 25. Juli 2015 Institut für Kernphysik (IKP) Folie 4
5 Permanent Electric Dipole Moments (EDM) of nondegenerate fundamental systems (particles): F. Wilczek, Jan Juli 2015 Institut für Kernphysik (IKP) Folie 5
6 Multiple experimental input is required to disentangle the fundamental source(s) of EDMs: Jordy de Vries, Juli 2015 Institut für Kernphysik (IKP) Folie 6
7 Multiple experimental input is required to disentangle the fundamental source(s) of EDMs: P. Harris, K. Kirch, July Juli 2015 Institut für Kernphysik (IKP) Folie 7
8 Experimental status of EDMs: best limits for bare nucleon (n, p), lepton (e, m), diamagnetic atom ( 199 Hg), paramagnetic atom ( 205 Tl) and molecules (YbF, ThO): Ongoing/future projects ThO d e < 8.7 x ecm 90% C.L. factor 10 in next 10 yrs P. Harris, K. Kirch, July Juli 2015 Institut für Kernphysik (IKP) Folie 8
9 nedms: past, ongoing and future experiments: Adapted from: Nature, Vol 482 (2012) UCN: reactors (ILL, FRM II), accelerators (PSI, ) Future goal: sensitivity limit: (few times) ecm 25. Juli 2015 Institut für Kernphysik (IKP) Folie 9
10 Experimental status of EDMs: best limits for bare nucleon (n, p), lepton (e, m), diamagnetic atom ( 199 Hg), paramagnetic atom ( 205 Tl) and molecules (YbF, ThO): Ongoing/future projects Direct measurements: sredm ThO d e < 8.7 x ecm 90% C.L. factor 10 in next 10 yrs P. Harris, K. Kirch, July Juli 2015 Institut für Kernphysik (IKP) Folie 10
11 Charged particle (p, d) EDMs: principle of experiment: Inject polarized particles into a storage ring Apply radial electric field E Non-zero EDM spin rotation out of the plane 25. Juli 2015 Institut für Kernphysik (IKP) Folie 11
12 Charged particle (p, d) EDMs: principal challenges Spin motion also due to MDM B = 0 all-electric ring Magic momentum spin in momentum direction Spin motion equation ( Thomas BMT ) shows: ds/dt is due to EDM (only for protons, G > 0)) For deuterons (and 3 He) [with G < 0] combined E-B benders required magic mom. 25. Juli 2015 Institut für Kernphysik (IKP) Folie 12
13 Charged particle (p, d) EDMs: technological challenges EDMs are very small ( ) systematics, fake EDM effects Current solution: dedicated precision storage ring with two beams (CW, CCW) goal: sensitivity of e cm (stepwise approach: R&D, precursor, sredm-ring) 25. Juli 2015 Institut für Kernphysik (IKP) Folie 13
14 Charged particle (p, d) EDMs: key technologies Polarimetry detect spin rotation of 1 nrad/s Spin coherence time at least 1000 s E/B benders high electric fields > 10 MV/m Beam position relative measurement; feedback Shielding of external fields ( ) Talk by Mei Bai (today, 12:30 h, Accelerator session) Accelerator physics challenges in EDM measurements Best place to pursue sredm: COSY at Forschungszentrum Jülich (FZJ), Jülich 25. Juli 2015 Institut für Kernphysik (IKP) Folie 14
15 Side remark: recent results obtained at COSY spin coherence time SCT of a few 1000 s spin tune measurement: 25. Juli 2015 Institut für Kernphysik (IKP) Folie 15
16 Charged particle (p, d) EDMs: Project at Jülich Cooler Synchroton COSY JEDI Collaboration Perfect R&D machine Precursor expt. in 2017/18 Injector for dedicated ring ~ 110 (11 countries) Embedded in JARA Fame Welcome to join! 25. Juli 2015 Institut für Kernphysik (IKP) Folie 16
17 25. Juli 2015 Institut für Kernphysik (IKP) Folie 17
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