EuCARD-2 is co-funded by the partners and the European Commission under Capacities 7th Framework Programme, Grant Agreement 312453 Highlights and roadmap.

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Presentation transcript:

EuCARD-2 is co-funded by the partners and the European Commission under Capacities 7th Framework Programme, Grant Agreement Highlights and roadmap from EuCARD-2 XPOL Kurt Aulenbacher

Content XPOL Deliverables: One workshop per year So far three workshops took place: participants.. General remark: Spin at accelerators is a “fundamental” science issue. - particle physics meets accelerator people..perhaps more directly than in other cases… -But: Almost no applied Physics yet (  small community!)

23 Participants: -national research centers (DESY,BNL) & - Many german universities (Bonn, Heidelberg, Munich, Mainz, ) Highlights: high energy circular proton machines, polarized positron source, “Spin at work” (in linear collider) XPOL workshop Spin optimization at Lepton accelerators (Mainz, February, )

23 Participants: -national research centers (DESY,BNL) & - Many german universities (Bonn, Heidelberg, Munich, Mainz, ) Highlights: high energy circular proton machines, polarized positron source, “Spin at work” (in linear collider) XPOL workshop Spin optimization at Lepton accelerators (Mainz, February, )

5

6

G. Moortgat Pick 7 (Polarized) Positron Bunch population not Completely safe…

8 Positron source is located at the end of the electron linac required positron yield Y = 1.5 e+/e- Superconducting helical undulator – 231m maximum active length  positron beam is polarized Photon-Collimator to increase e+ pol – Removes part of photon beam with lower polarization e+ Production Target, 400m downstream the undulator Positron Capture: OMD (Optical Matching Device) – Pulsed flux concentrator

EuCARD Workshop, Mainz Positron Target Material: Titanium alloy Ti-6%Al-4%V Thickness: 0.4 X 0 (1.4 cm) Incident photon spot size on target:  2 mm (rms) (Ee- = 150GeV) ~ 1.2 mm (Ee- = 250GeV) Power deposition in target: TDR 5-7% (~4kW) small beam size  high peak energy density  spinning wheel to avoid damage due to high energy deposition density – 2000 r.p.m. (100m/s) – Diameter: 1m – Wheel is in vacuum – water-cooled Potential problems – Stress waves due to cyclic heat load  target lifetime – High peak energy deposition – Eddy currents – rotating vacuum seals to be confirmed suitable (design and prototyping is ~ongoing) S. Riemann

EuCARD Workshop, Mainz Positron Target S. Riemann „EUCARD SPIN-OFF“: POSITAR Experiment „MIMIC“ impact of photon beam by ionization loss due to focussed electron beam at several MeV. High repetition rate possible at c.w. electron accelerators.  1 day of operation at MAMI mimicks 1 year operation at the ILC. (first experiment on Titanium alloy 2/2016)

11 Participants: 27 Particle physics meets storage ring! (No collider!) US (BNL, CORNELL), Korea (CAPP), Germany (COSY-Jülich), Italy (Ferrara), Russia (Dubna), Highlights: Spin coherence, non-invasive effective polarimetry, Particle physics without collisions! XPOL workshop Search for the electron EDM in an electrostatic storage ring. Mainz, September

12 Electric Dipole Moment=EDM EDM‘s imply CP-violation (bigger than present standard model)  So far only effective experiments with NEUTRAL (composite) systems (exception: neutron)  Storage rings allow for measurement on truely elementary systems (p, e,  )  Electric

13 Assuming CPT is invariant, this implies that CP is violated too…

Electroweak Baryogenises GUT SUSY J.M.Pendlebury and E.A. Hinds, NIMA 440 (2000) 471 e-cm Gray: Neutron Red: Electron n current n target Sensitivity to Rule on Several New Models e current e target p, d target If found it could explain Baryogenesis (p, d, n, 3 He) If found it could explain Baryogenesis (p, d, n, 3 He) Much higher physics reach than LHC; complementary Much higher physics reach than LHC; complementary Statistics limited 1 st upgrade Electron EDM new physics reach: 1-3 TeV

15 A. Lehrach, FZJ

16 Momentum vector Spin vector E E E E at the magic momentum

17 Signal can be mimicked by radial magnetic fields  eliminate those by all electric ring operaqting at „magic“ momentum („frozen spin“ points always in direction of motion) Hadrons promise easier success, but require much more expensive ring Problem with electron: efficiency of Polarimetry. Way out: Transfre from intensity to frequency measurement (Talman)

18

19 XPOL workshop Polarization issues in future high energy circular colliders Rome, April Particpants (China, Germany, Japan, Switzerland, Russia, US,) Small, but extremely intense meeting with vivid Discussions… Highlights: Vertical polarization In fcc-ee  energy calibration (Ginafelice, Hillert, Koop, Fcc-hh: polarization not hopeless (Ptytsin) internal Target also (Lenisa) Again,polarimetry is the key…

E Gianfelice (Fermilab): Long self-polariation time requires damping wigglers if 10% polarization required (energy measure,ent due to resonant depolarization)  senstivity of compton scattering better 1% (Hillert?) 20

21 Next XPOL workshop End of 2016 New venues in polarimetry Beam Polarimetry is the key issue for several project in acclerator based research -fcc-ee energy calibration -eEDM determination („Resonant polarimter“) - -Highly accurate polarimeters for precision observables (Hydro Moller completely polarized internal target, double scattering, )