Mitglied der HelmholtzGemeinschaft EDM Theory and Experiment Search

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Mitglied der Helmholtz-Gemeinschaft EDM (Theory and) Experiment: Search for new Physics beyond the Standard

Mitglied der Helmholtz-Gemeinschaft EDM (Theory and) Experiment: Search for new Physics beyond the Standard Model December 5, 2012 Frank Rathmann (on behalf of the BNL-EDM and JEDI collaborations) DISCRETE 2012, IST, Lisboa, Portugal

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches §

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches § Concepts for dedicated Storage Ring searches § Technological challenges § Precursor Experiments § Timelines of projects § Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 2

Introduction: The big challenges Conventional HEP wisdom, but there is more than that …

Introduction: The big challenges Conventional HEP wisdom, but there is more than that … f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 3

Introduction: Physics Frontiers I en t n ity plex Com (In-)stability of the proton

Introduction: Physics Frontiers I en t n ity plex Com (In-)stability of the proton f. rathmann@fz-juelich. de rg y Frontiers of Physical Sciences Precision mic y t i s En e Cos Secrets of neutrinos Search for the origin of mass („Higgs“), SUSY Quest for „Dark Matter“ and „Dark Energy“ EDM Theory and Experiment: Search for new Physics beyond the Standard Model 4

Introduction: Precision Frontier ESPP, Cracow, September 2012 A most promising additional frontier: Precision f.

Introduction: Precision Frontier ESPP, Cracow, September 2012 A most promising additional frontier: Precision f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 5

Introduction: Precision Frontier Example: Neutron (n. EDM) Adapted from: Nature, Vol 482 (2012) Search

Introduction: Precision Frontier Example: Neutron (n. EDM) Adapted from: Nature, Vol 482 (2012) Search for Electric Dipole Moments (EDM) of fundamental particles f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 6

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches §

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches § Concepts for dedicated Storage Ring searches § Technological challenges § Precursor Experiments § Timelines of projects § Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 7

Physics: Fundamental Particles Do particles (e. g. , electron, nucleon) have an EDM? f.

Physics: Fundamental Particles Do particles (e. g. , electron, nucleon) have an EDM? f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 8

EDMs: Discrete Symmetries Not Charge symmetric Permanent EDMs violate P and T. Assuming CPT

EDMs: Discrete Symmetries Not Charge symmetric Permanent EDMs violate P and T. Assuming CPT to hold, CP violated also. f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 9

EDMs: Why is CPV so interesting? • CPV in the SM points to physics

EDMs: Why is CPV so interesting? • CPV in the SM points to physics we do not understand • CPV is highly sensitive to physics beyond the SM (New Physics) • CPV is accessible to a wide range of experiments • New source of CPV beyond the SM required for baryogenesis Physics beyond the Standard Model (BSM) f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 10

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches §

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches § Concepts for dedicated Storage Ring searches § Technological challenges § Precursor Experiments § Timelines of projects § Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 11

Physics: What caused the Baryon asymmetry? Carina Nebula: Largest-seen star-birth regions in the galaxy

Physics: What caused the Baryon asymmetry? Carina Nebula: Largest-seen star-birth regions in the galaxy What happened to the antimatter? Observed WMAP+COBE (2003) SM exp. Sakharov (1967): Three conditions for baryogenesis 1. B number conservation violated sufficiently strongly 2. C and CP violated, B and anti-Bs with different rates 3. Evolution of universe outside thermal equilibrium The mystery of the missing antimatter (the puzzle of our existence) f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 12

Physics: Potential of EDMs N. Arkani-Hamed (IAS, Princeton) at Intensity Frontier WS, USA (2011)

Physics: Potential of EDMs N. Arkani-Hamed (IAS, Princeton) at Intensity Frontier WS, USA (2011) f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 13

Physics: Potential of EDMs G. Isidori at ESPP Open Symposium, Cracow (Sept. 2012) f.

Physics: Potential of EDMs G. Isidori at ESPP Open Symposium, Cracow (Sept. 2012) f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 14

Physics: Potential of EDMs J. M. Pendlebury: „n. EDM has killed more theories than

Physics: Potential of EDMs J. M. Pendlebury: „n. EDM has killed more theories than any other single expt. “ f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 15

Physics: Limits for Electric Dipole Moments Particle/Atom Current EDM Limit Future Goal Electron Neutron

Physics: Limits for Electric Dipole Moments Particle/Atom Current EDM Limit Future Goal Electron Neutron Proton Deuteron ? Huge efforts underway worldwide to improve limits / find EDMs f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 16

Physics: Ongoing/planned Searches new P. Harris, K. Kirch … A huge worldwide effort f.

Physics: Ongoing/planned Searches new P. Harris, K. Kirch … A huge worldwide effort f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 17

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches §

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches § Concepts for dedicated Storage Ring searches § Technological challenges § Precursor Experiments § Timelines of projects § Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 18

Principle: Frozen spin Method For transverse electric and magnetic fields in a ring (

Principle: Frozen spin Method For transverse electric and magnetic fields in a ring ( ), anomalous spin precession is described by Thomas-BMT equation: x (magic) Magic rings to measure EDMs of free charge particles f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 19

Principle: Rings for sr. EDM searches • Place particles in a storage ring •

Principle: Rings for sr. EDM searches • Place particles in a storage ring • Align spin along momentum („Freeze“ horizontal spin precession) • Search for time development of vertical polarization New Method to measure EDMs of free charge particles: Magic rings with spin frozen along momentum f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 20

EDMs: Storage ring projects p. EDM in all electric ring at BNL or at

EDMs: Storage ring projects p. EDM in all electric ring at BNL or at FNAL Jülich, focus on deuterons, or a combined machine (from R. Talman) CW and CCW propagating beams (from A. Lehrach) Two projects: US (BNL or FNAL) and Europe (FZJ) f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 21

Beat systematics: BNL Proposal 2 beams simultaneously rotating in an all electric ring (cw,

Beat systematics: BNL Proposal 2 beams simultaneously rotating in an all electric ring (cw, ccw) CW & CCW beams cancels systematic effects CW CCW Sokolov-Ternov Gravitation Status: Approved BNL-Proposal Submitted to DOE Goal for protons Many technological challenges need to be met f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 22

Principle: Magic Storage ring A magic storage ring for protons (electrostatic), deuterons, … B

Principle: Magic Storage ring A magic storage ring for protons (electrostatic), deuterons, … B particle proton deuteron f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 23

CCW & CCW with magnetic field: Richard Talmans concept for a Jülich all-in-one machine

CCW & CCW with magnetic field: Richard Talmans concept for a Jülich all-in-one machine Iron-free, current-only, magnetic bending, eliminates hysteresis B A A Configuration generates close-to-perfect vertical B field f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model B 24

Magic ring: Jülich all-in-one machine (R. Talmans concept ) B particle proton deuteron Very

Magic ring: Jülich all-in-one machine (R. Talmans concept ) B particle proton deuteron Very compact machines possible for sr. EDM searches f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 25

EDMs – Sensitivity Reach EDM search in charged baryon (systems) p. EDM d. EDM

EDMs – Sensitivity Reach EDM search in charged baryon (systems) p. EDM d. EDM Adapted from: Nature, Vol 482 (2012) No direct measurements for proton and deuteron EDM yet ! f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 26

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches §

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches § Concepts for dedicated Storage Ring Searches § Technological challenges § Precursor Experiments § Timelines of projects § Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 27

sr. EDM searches: Technogical challenges These issues must be addressed experimentally at existing facilities

sr. EDM searches: Technogical challenges These issues must be addressed experimentally at existing facilities f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 28

Challenge: Electric field for magic rings Challenge to produce large electric field gradients f.

Challenge: Electric field for magic rings Challenge to produce large electric field gradients f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 29

Challenge: Niobium electrodes DPP stainless steel fine-grain Nb Show one slide on JLAB data

Challenge: Niobium electrodes DPP stainless steel fine-grain Nb Show one slide on JLAB data HV devices large-grain Nb Nb single-crystal Nb Large-grain Nb at plate separation of a few cm yields ~20 MV/m f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 30

Challenge: Spin coherence time Spin closed orbit one particle with magnetic moment makes one

Challenge: Spin coherence time Spin closed orbit one particle with magnetic moment makes one turn “spin closed orbit vector” “spin tune” stable polarization ring A f. rathmann@fz-juelich. de if ║ EDM Theory and Experiment: Search for new Physics beyond the Standard Model 31

Challenge: Spin coherence time Polarization not affected! At injection all spin vectors aligned (coherent)

Challenge: Spin coherence time Polarization not affected! At injection all spin vectors aligned (coherent) After some time, spin vectors get out of phase and fully populate the cone Longitudinal polarization vanishes! At injection all spin vectors aligned Later, spin vectors are out of phase in the horizontal plane In an EDM machine with frozen spin, observation time is limited. f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 32

Challenge: SCT stimates (N. N. Nikolaev) One source of spin coherence are random variations

Challenge: SCT stimates (N. N. Nikolaev) One source of spin coherence are random variations of the spin tune due to the momentum spread in the beam and is randomized by e. g. , electron cooling Estimate: Spin coherence time for deuterons may be ������ × larger than for protons f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 33

EDM at COSY: COoler SYnchrotron COSY Injector cyclotron f. rathmann@fz-juelich. de … …the an

EDM at COSY: COoler SYnchrotron COSY Injector cyclotron f. rathmann@fz-juelich. de … …the an spin-physics ideal starting machine point forahadron sr. EDMphysics search EDM Theory and Experiment: Search for new Physics beyond the Standard Model 34

Challenge: First measurement of SCT 2011 Test measurements at COSY Polarimetry: Spin coherence time:

Challenge: First measurement of SCT 2011 Test measurements at COSY Polarimetry: Spin coherence time: decoherence oscillation time capture f. rathmann@fz-juelich. de from Ed Stephenson and Greta Guidoboni EDM Theory and Experiment: Search for new Physics beyond the Standard Model 35

Challenge: SCT recent achievements Result from 2012 run from Ed Stephenson and Greta Guidoboni

Challenge: SCT recent achievements Result from 2012 run from Ed Stephenson and Greta Guidoboni f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 36

Challenge: Polarimetry Beam polarimetry at the ppm level achieved for deuteron beams f. rathmann@fz-juelich.

Challenge: Polarimetry Beam polarimetry at the ppm level achieved for deuteron beams f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 37

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches §

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches § Concepts for dedicated Storage Ring Searches § Technological challenges § Precursor Experiments § Timelines of projects § Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 38

Precursor experiments: RF methods Methods based on making the spin precession in the machine

Precursor experiments: RF methods Methods based on making the spin precession in the machine resonant with the orbit motion Two ways: 1. Use an RF device that operates on some harmonics of the spin precession frequency 2. Operate ring on an imperfection resonance Use existing magnetic machines for first direct EDM measurements f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 39

Precursor experiments: Resonance Method with „magic“ RF Wien filter Avoids coherent betatron oscillations of

Precursor experiments: Resonance Method with „magic“ RF Wien filter Avoids coherent betatron oscillations of beam. Radial RF-E and vertical RF-B fields to observe spin rotation due to EDM Approach pursued for a first direct measurement at COSY. Indirect EDM effect RF E(B)-field stored d Polarimeter (dp elastic) f. rathmann@fz-juelich. de In-plane polarization Tilt of precession plane due to EDM Observable: Accumulation of vertical polarization during spin coherence time EDM Theory and Experiment: Search for new Physics beyond the Standard Model 40

Precursor experiments: Resonance Method for deuterons at COSY f. rathmann@fz-juelich. de EDM Theory and

Precursor experiments: Resonance Method for deuterons at COSY f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 41

Precursor experiments: Resonance Method for deuterons at COSY f. rathmann@fz-juelich. de EDM Theory and

Precursor experiments: Resonance Method for deuterons at COSY f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 42

Precursor experiments: Resonance EDM measurement with a static Wien filter Spin rotation in phase

Precursor experiments: Resonance EDM measurement with a static Wien filter Spin rotation in phase with orbit motion Similar accumulation of EDM signal, systematics more difficult, strength of imperfection resonance must be suppressed by closed-orbit corrections. f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 43

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches §

Outline § § Introduction Electric Dipole Moments Physics Impact Charged particle EDM searches § Concepts for dedicated Storage Ring Searches § Technological challenges § Precursor Experiments § Timelines of projects § Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 44

Timeline: BNL EDM Technically driven for all-electric p. EDM 12 13 14 15 16

Timeline: BNL EDM Technically driven for all-electric p. EDM 12 13 14 15 16 17 18 19 20 21 Two years R&D/preparation One year final ring design Two years ring/beam-line construction Two years installation One year “string test” f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 45

Timeline: Stepwise approach all-in-one machine for JEDI Step Aim / Scientific goal 1 Device

Timeline: Stepwise approach all-in-one machine for JEDI Step Aim / Scientific goal 1 Device / Tool Storage ring Spin coherence time studies Horizontal RF-B spin flipper COSY Systematic error studies Vertical RF-B spin flipper COSY upgrade Orbit control, magnets, … COSY RF-E(B) spin flipper Modified COSY Common magneticelectrostatic deflectors Dedicated ring 2 3 Dedicated ring 4 Time scale: f. rathmann@fz-juelich. de Steps 1 and 2: < 5 years Steps 3 and 4: > 5 years EDM Theory and Experiment: Search for new Physics beyond the Standard Model 46

Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the

Conclusion f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 47

Georg Christoph Lichtenberg (1742 -1799) “Man muß etwas Neues machen, um etwas Neues zu

Georg Christoph Lichtenberg (1742 -1799) “Man muß etwas Neues machen, um etwas Neues zu sehen. ” “You have to make (create) something new, if you want to see something new” f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 48

Spares f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the

Spares f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 49

sr. EDM cooperations International sr. EDM Network Institutional (Mo. U) and Personal (Spokespersons …)

sr. EDM cooperations International sr. EDM Network Institutional (Mo. U) and Personal (Spokespersons …) Cooperation, Coordination sr. EDM Collaboration (BNL) JEDI Collaboration (FZJ) (spokesperson Yannis Semertzidis) (spokespersons: A. Lehrach, J. Pretz, F. R. ) Common R&D RHIC Beam Position Monitors (…) EDM-at-COSY Polarimetry Spin Coherence Time Cooling Spin Tracking (…) Study Group DOE-Proposal (submitted) CD 0, 1, … p. EDM Ring at BNL f. rathmann@fz-juelich. de First direct measurement Ring Design HGF Application(s) JEDI EDM Theory and Experiment: Search for new Physics beyond the Standard Model 50

EDM Workshop at ECT* (Trento) October 1 -5, 2012 http: //www. ectstar. eu/ Organizing

EDM Workshop at ECT* (Trento) October 1 -5, 2012 http: //www. ectstar. eu/ Organizing committee - Jülich Hans Ströher h. stroeher@fz-juelich. de Frank Rathmann f. rathmann@fz-juelich. de Andreas Wirzba a. wirzba@fz-juelich. de - Brookhaven Mei Bai mbai@bnl. gov William Marciano marciano@bnl. gov Yannis Semertzidis yannis@bnl. gov f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 51

Magnetic moment, spin, g and G Nuclear magneton particle proton deuteron 3 He f.

Magnetic moment, spin, g and G Nuclear magneton particle proton deuteron 3 He f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 52

Operation of „magic“ RF Wien filter f. rathmann@fz-juelich. de EDM Theory and Experiment: Search

Operation of „magic“ RF Wien filter f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 53

Simulation of resonance Method with Magic Wien filter for deuterons at COSY f. rathmann@fz-juelich.

Simulation of resonance Method with Magic Wien filter for deuterons at COSY f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 54

Why also EDMs of protons and deuterons? Proton and deuteron EDM experiments may provide

Why also EDMs of protons and deuterons? Proton and deuteron EDM experiments may provide one order higher sensitivity. In particular the deuteron may provide a much higher sensitivity than protons. f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 55

History of neutron EDM limits • Smith, Purcell, Ramsey PR 108, 120 (1957) •

History of neutron EDM limits • Smith, Purcell, Ramsey PR 108, 120 (1957) • RAL-Sussex-ILL (dn 2. 9 10 -26 e cm) PRL 97, 131801 (2006) Adopted from K. Kirch f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 56

Magic condition: Protons magic energy f. rathmann@fz-juelich. de magic energy EDM Theory and Experiment:

Magic condition: Protons magic energy f. rathmann@fz-juelich. de magic energy EDM Theory and Experiment: Search for new Physics beyond the Standard Model 57

Magic condition: Deuterons f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics

Magic condition: Deuterons f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 58

Magic condition: Helions f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics

Magic condition: Helions f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 59

Some polarimetry issues p. C and d. C polarimetry is the currently favored approach

Some polarimetry issues p. C and d. C polarimetry is the currently favored approach for the p. EDM experiment at BNL f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 60

Exploit observables that depend on beam and target polarization f. rathmann@fz-juelich. de EDM Theory

Exploit observables that depend on beam and target polarization f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 61

Detector CW CCW cell f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new

Detector CW CCW cell f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 62

Suggestion 2: Use colliding beam from external source Detector Polarized ion source (~10 Me.

Suggestion 2: Use colliding beam from external source Detector Polarized ion source (~10 Me. V) • Collide two external beams with cw and ccw stored beams. • Energy could be tuned to match detector acceptance. • Polarization components of probing low-energy beam can be made large, would be selected by spin rotators in the transmission lines. • Luminosity estimates necessary f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 63

Suggestion 3: Use directly reactions from colliding beams Detector CW f. rathmann@fz-juelich. de CCW

Suggestion 3: Use directly reactions from colliding beams Detector CW f. rathmann@fz-juelich. de CCW EDM Theory and Experiment: Search for new Physics beyond the Standard Model 64

Luminosity estimate for the collider option f. rathmann@fz-juelich. de EDM Theory and Experiment: Search

Luminosity estimate for the collider option f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 65

Resonance Method with RF E-fields spin precession governed by: RF E-field (* rest frame)

Resonance Method with RF E-fields spin precession governed by: RF E-field (* rest frame) vertical polarization stored d Polarimeter (dp elastic) • But: Flipping fields will lead to coherent betatron oscillations, with hard to handle systematics. EDM Theory and Experiment: Search for new Physics beyond the Standard f. rathmann@fz-juelich. de Model 66

Simulation of resonance Method with RF E-fields for deuterons at COSY Constant E-field Number

Simulation of resonance Method with RF E-fields for deuterons at COSY Constant E-field Number of turns f. rathmann@fz-juelich. de Number of turns EDM Theory and Experiment: Search for new Physics beyond the Standard Model 67

Simulation of resonance Method with RF E-fields for deuterons at COSY Number of turns

Simulation of resonance Method with RF E-fields for deuterons at COSY Number of turns f. rathmann@fz-juelich. de EDM Theory and Experiment: Search for new Physics beyond the Standard Model 68

Symmetries Physical laws are invariant under certain transformations. Parity: T-Symmetry: C-parity (or Charge parity):

Symmetries Physical laws are invariant under certain transformations. Parity: T-Symmetry: C-parity (or Charge parity): f. rathmann@fz-juelich. de Changes sign of all quantized charges • electrical charge, • baryon number, • lepton number, • flavor charges, • Isospin (3 rd-component) EDM Theory and Experiment: Search for new Physics beyond the Standard Model 69