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E166: Polarized Positrons & Polarimetry K. Peter Schüler ILC: - why polarized positrons - e+ source options - undulator source scheme E166 - proof-of-principle.

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Presentation on theme: "E166: Polarized Positrons & Polarimetry K. Peter Schüler ILC: - why polarized positrons - e+ source options - undulator source scheme E166 - proof-of-principle."— Presentation transcript:

1 E166: Polarized Positrons & Polarimetry K. Peter Schüler ILC: - why polarized positrons - e+ source options - undulator source scheme E166 - proof-of-principle demonstration of the undulator method - undulator basics - transmission polarimetry - G EANT 4 polarization upgrade results & conclusions E166: Polarized Positrons & Polarimetry K. Peter Schüler (DESY) - on behalf of the E166 Collaboration JPOS 09 at Jefferson Lab 25-27 March 2009

2 ILC: why polarized positrons? 2 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler SLC as precursor of the ILC very successfully employed polarized electrons, but not polarized positrons. What does the ILC gain from polarized positrons? longitudinally polarized beams: can enhance or suppress processes!

3 why polarized positrons? 3 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler effective polarization in s-channel (e+e-  γ/Z) annihilation: positron polarization can significantly increase precision in measurement of A LR

4 4 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler why polarized positrons? Supersymmetry: Selectron Pair Production positron polarization is required for separation of RR from LR pairs

5 5 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler why polarized positrons? can effectively enhance or suppress processes improved signal/background ratio higher effective polarization and precision in A LR asymmetry unique understanding of non-standard couplings explore new physics (e.g. extra dim.) with transverse beam pol. G. Moortgat-Pick et al., Physics Reports 460 (2008) 131-243 CERN-PH-TH-2005-036, SLAC-PUB-11087, arXiv: hep-ph/0507011

6 e + source options for the ILC 6 existing/proposed positron sources: ← ILC 3 Concepts: large amount of charge req‘d ! ‚conventional‘ laser Compton based undulator-based JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

7 undulator source 7 PRO: photoprod. in thin target 0.4 X 0 Ti-alloy  lower e+ beam emittance less energy deposition in target (1/5) and AMD (1/10) less neutron induced activation (1/16) no multiplexing & accumulation req‘d polarized positrons CON: need high-energy electron drive beam (coupled e+/e- operation) long undulator (150-300 m) req‘d positron beam profile JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

8 undulator source scheme for ILC 8 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler undulator is chosen baseline scheme for the positron source (although initially at less than full length) expect initial e+ polarization of ~ 30% Compton based e+ source has alternative status

9 E166 – proof of principle demonstration of the undulator method 9 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

10 undulator basics 10 E166 ILC (RDR) electron beam energy (GeV) 46.6 150 field (T) 0.71 0.86 period (mm) 2.54 11.5 K value 0.17 0.92 photon energy  0 max (MeV) 7.9 10.0 beam aperture (mm) 0.89 5.85 active length (m) 1 147 M (no. of periods) 394 12800 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

11 undulator basics 11 E166 Photon SpectrumE166 Photon Polarization Spectrum:Angular Distribution:Polarization: first harmonic (dominating) expressions: E166 Photon Yield: = no. of photons per high-energy beam electron  0 max = 7.9 MeV JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

12 The E166 Experiment 12 2004/2005  setup and checkout Oct. 2005  4 weeks of data taking JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

13 E166 experimental setup 13 C1 – C4: photon collimation A1, A2: aerogel detectors S1, S2: silicon detectors GCAL: Si/W-calorimeter DM: electron beam dump magnets T1: g  e+ prod. target (0.2 X 0 W) T2: e+  g reconv. target (0.5 X 0 W) P1: e+ flux monitor (Silicon) CsI: Cesium Iodide calorimeter SL: solenoid lens J: movable jaws 4 – 8 MeV < 8 MeV JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

14 E166 photo gallery 14 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

15 transmission polarimetry 15 1.Compton Transmission Polarimetry for Low-Energy Photons relies on spin dependence of Compton effect in magnetized iron: 2.Positron Polarimetry: (a) transfer e+ polarization to photon via brems/annihilation process (b) then infer e+ polarization from measured photon pol. as in method 1. JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

16 16 analyzer magnets: overview active volume Photon Analyzer: 50 mm dia. x 150 mm long Positron Analyzer: 50 mm dia. x 75 mm long P e ≈ 0.07 ΔP e /P e ~ 0.03 electron polarization of the iron: M = (B–B 0 )/  0  magnetization n = electron density μ B = Bohr magneton g‘ = magneto-mechanical factor JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

17 17 analyzer magnets CsI-Detector e+ Analyzer Pickup Coils e+ Analyzer  Analyzer JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

18 18 electron polarization of the iron  P e /P e ~ 2% JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler P e ~ 0.07

19 19 Simulations JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler GEANT4 upgrade for spin-dependent e/m processes: gammas: - gamma conversion - Compton scattering - photo-electric effect electrons & positrons: - multiple scattering - ionization - bremsstrahlung polarization tranfer -  Y e+/e- - e+/e- Y  polarimetry - Compton scattering - Bhabha scattering - Moller scattering - positron annihilation in flight e+/e- spectra at production target e+/e- polarization & analyzing power

20 20 photon asymmetries detector asymmetry  (%)  measured predicted S2 (silicon) 3.88 E 0.12 E 0.63 3.1 A2 (aerogel) 3.31 E 0.06 E 0.16 3.6 GCAL (Si/W-calo) 3.67 E 0.07 E 0.40 3.4 reasonable agreement with simulation results based on theoretical undulator polarization spectrum and detector response functions but no detailed spectral shape analysis possible JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

21 21 positron measurements exp. asymmetry of ~1% expected in CsI large background from e- beam halo req‘s equal amount of undulator „on“ and „off“ statistics normalization to P1 detector avoids false asymmetries from flip-correlated beam shifts JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

22 energy deposition in CsI crystals 22 good signal/background separation in central crystal background from e- beam halo hitting the undulator undulator on/off measurements taken on alternating machine pulses for effective background subtraction undulator on: signal + background undulator off: background JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

23 23 positron asymmetries JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

24 24 positron asymmetries JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

25 results: beam polarization 25 = analyzing power from simulations = electron polarization of the iron JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

26 26 conclusions successful demonstration of the undulator method undulator functioned as predicted successful polarimetry of low-energy  and e+ confirmed expected γ  e+ spin-transfer mechanism measured high positron polarization with ~ 85% max. JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

27 27 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler long paper (66 pages) about to be submitted to NIM PRL 100, 210801 (2008), G. Alexander et al.: published results

28 28 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler why polarized positrons? Transverse Beam Polarization: Gravity in Extra Dimensions: expect significant asymmetric deviations from SM in the azimuthal distributions T. G. Rizzo, JHEP 0302 (2003) 008 [arXiv:hep-ph/0211374]; JHEP 0308 (2003) 051 [arXiv:hep-ph/0306283].

29 29 conventional positron source (as used for SLC at SLAC) PRO: established technology (although not at req‘d level) CON: pushing technical limits of target materials; req‘s multiple targets and beamlines; very high activation levels no polarization option thick W-Re target: strong multiple scattering, less efficient e+ capture JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

30 30 spin and magnetization g‘ = magneto-mechanical factor: obtained from Einstein - de Haas type experiments, related to gyromagnetic ratio: γ = (g‘/2) ∙ (e/m) the principle … and its ultimate implementation (Scott 1962) g‘ = 1.919 ± 0.002 for pure iron i.e. orbital effects contribute about 4% Note: g‘ = 2  M s / M = 1 (pure spin magnetization) γ = e/m g‘ = 1  M s / M = 0 (pure orbit magnetization) γ = ½ (e/m) JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

31 31 field distribution modeling (Vector Fields OPERA-2d) R = 0 mm 10 15 22.5 B z (T) Z (mm) longitudinal field distribution: B z (R,Z) field drops gradually towards the ends: L eff / L < 1 center end 20 5 JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

32 32 field distribution in 2d (Vector Fields OPERA-2d) longitudinal field distribution: B z (R,Z) (shown for one quadrant) R (mm) Z (mm) JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

33 33 flux measurements: measure voltage transients in pickup coils upon current reversals Positron Analyzer (-60  +60 amps) voltage transient JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

34 34 flux and field measurements: results Note: polarimetry was always done at full saturation over the central region (±60A) Z = 0 (center) JPOS 09 at Jefferson Lab 25-27 March 2009 E166: Polarized Positrons & Polarimetry K. Peter Schüler

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