possibility of antiproton polarization by spin transfer 1 antiproton polarization by spin- exchange...
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Possibility of antiproton polarization by Spin transfer
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Antiproton Polarization by Spin-exchange from Positrons?
PST2007 Brookhaven
September,10,2007
Kurt Aulenbacher
Institut für Kernphysik der Uni Mainz
Possibility of antiproton polarization by Spin transfer
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Outline
1. Pol-Antiprotons (pbar): Why?
2. Pol-pbar: Status.
3. Compact polarized positron sources
Possibility of antiproton polarization by Spin transfer
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Pol pbar:Why?
For the FAIR facility pbar-polarization could play the same role as pol.electrons did for SLAC, JLAB, MAMI.
….but so far no efficient way of polarizing pbar.
Antiproton-storage ring
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Ultrashort History of pbar-polarization schemes
1. 1992: FILTEX-experiment:Spin filtering (Spin dependent nuclear forces) in p (\vec p)-scattering demonstrated (polarized gas target in p-storage ring at 23 MeV). Filter cross section smaller than expected.
2. 1994: Horowitz and Mayer calculate large spin dependent cross section (Spin transfer coefficient‘ (STC)) in p(\vec e) scattering (1barn cross section at 5MeV)
3 2007: Distorted wave calculation of STC with realistic Coulomb wave functions by Arenhövel for very low relative velocities of lepton and pbar. No major increase of effect for electron/pbar but huge increase of STC for positron/electron scattering
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Small velocities
Advantage w.r.t. internal target: i) Increased beam life time,ii) directly applicable at all interesting pbar energies.iii) predictions may be tested conveniently in e-/proton interaction BUT:Even with high brightness source (30 A/cm2 over 1m at 4mm2 beam area), The cross section enhancement must make up for factor ~105 with respect to storage cell experiment (1barn cross section)
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A ‚huge‘ effect
• Non-screened interaction!• slow positrons are attracted to pbar• Interference between Coulomb- and Hyperfineamplitude creates large STC.
Reasons to worry:
1) Depolarization cross section at EH~1eV < 1010 barn (i.e. COSY exp.)2) Mayer (Aug. 2007) points out that STC may not necessarily lead to polarization of the pbar beam.
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STC is ‚not really‘ polarizing
Important is the Spin exchange: +- -+i.e. by Hyperfine interaction in Semiconductors.
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Preliminary Conclusion
1. Theoretical calculation of Spin exchange is underway.
2. Experiment at COSY Julich in Fall 2007probably has sensitivity to detect ~106 barns spin exchange c.s.
3. The smaller the cross section the more complicated the positronsource will have to be. What are the options?
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Compact polarized e+ sources
Generation Mechanism,i.e. radioactivity,Pair production
Low brightness: High average energy,Large spread in energy, Position, and momentum
Increase brightness by dissipative process
Decelleration:Dissipation by multiple scattering
Acceleration: Dissipation by syncrotron radiation
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Principle of moderation
•Absorber necessary in order to shift high intensity/high polarization part of -Spektrum to ~10keV.
•Absorber also suppresses positrons which large emission angles!
•~10keV Positrons are stopped close to moderator surface and escape because of negative positron work function.
•Escaping Positrons have thermal energy spread (!!)
J. van House et al. Phys. Rev. A 29,1 96 (1984)5*105/s at P=0.48 from Na-22. Efficiency: 2.5*10-4
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Possible d.c.-source parameters
Online C-11 production with Commercial superconducting Linac: 1.2 mA, 20MeV 1013 Bq source activity Expected Efficiency increase: factor 2compared to 1980-s experiment
Current: 5*109 e+/sPolarization: 0.7Energy width: <0.1eVNormalized beam emittance 1 mm mrad
Possibility of antiproton polarization by Spin transfer
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e+-Storage ring option
1. Profit from enhanced Beam current due to revolution frequency.
2. Conventional AG-storage ring offers beam lifetime of several seconds @1MeV
3. longitudinal spin stabilization with -rotating solenoid seems feasible.
4. Space charge limit 10mA.5. Aim at >3*105 stored particles (1
Mikroamp i.e 3 orders of mag. w.r.t. d.c. source)
6. Task: Produce 3*105 pol e+ in acceptance of 5keV*ns.
Antip ro to n b e a m in sto ra g e ring
Sp in tra nsfe r re g io n
C irc um fe re nc e ~ 14m (f = 21 M hz)re v
Kic ke r
Po la rize d e so urc e+So le no id fo r lo ng .
Sp in sta b iliza tio n
Possibility of antiproton polarization by Spin transfer
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General Idea:
eeSame as for the ILC sources….. ??
Possibility of antiproton polarization by Spin transfer
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T. Omori et al: PRL 96,114801 (2006)
Achieves about 103 polarized positrons with P=0.73 inside required acceptance.
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Compact Circularely polarized gamma source
1.) Conventional: Polarized Bremsstrahlung from polarized electrons (subsequent Brightness enhancement by moderation)2.) Unconventional: Laser accelerator(*) with small spread in all spacial dimensions +Compton backscattering from part of the drive laser pulse (tabletop e/Photon-collider(**).(Due to small initial pulse length no moderation needed)
*W.P. Leemans et al: Nature physics, 2, 696 (2006). **H Schwoerer et al. PhysRev.Lett., 96, 014802 (2006)
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Pulsed source with present day technology
• Generate circularely polarized gammas by Bremsstrahlung from polarized electrons
• If compared to the KEK-Ansatz we profit from the relatively long pulse length required.
• Will allow for compact (~15 m long) set up• only well established components
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A:Source: Pol. e pulse200keV,4sIpeak=5A
B:High charge r.f.-LINAC, 23MeV, Ipeak=1.7ANe-=4.3*1013
C;Conversion target1mm Tungsten(or liquid lead)
D:Positron energy (E) + Angular ()-selectionE=14.25MeVE=+-350keV,= 2deg.Conversion efficiency: 1=e+/e-=9*10-7
P=0.76
A B C D
E:Beam collimation
E
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F:Positron decelaration(r.f.-LINAC)14.25 to 1.75 MeV
Terminal with absorber/moderator (H) (at +1MV)and Buncher (I) (+ 0.99MV),reacceleration to ground potential (J)
Bunched e+ to storage ring E=1MeV, 50nsIpeak=2A
F G
G: Electrostaticdecelerationto Ekin= 1 MeV at terminal
H I J
{E
Moderator efficiency:2=1.4%.
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Expected parameters for pulsed source (conventional version)
• Bunch charge 6*105 (from 1.2*1014 pol. electrons)
• Polarization 0.76
• normalized emittance 9 mm mrad
• longitudinal phase space 4 keV*ns
• Current in storage ring 2 A.
• repetition rate 10 Hertz no lifetime problem for polarized electron source.
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Can it be improved even further?
Antip ro to n b e a m in sto ra g e ring
Sp in tra nsfe r re g io n
C irc um fe re nc e ~ 14m (f = 21 M hz)re v
Kic ke r
Po la rize d e so urc e+So le no id fo r lo ng .
Sp in sta b iliza tio n
1. Increase storage time (and space charge limit)by longitudinal (toroidal)Magnetfield (Stellatron)2.) The Stellatron (aka LEPTA)is intended for electron cooling of stored positron beams! with ~mA current. 3.) But: Not investigated: i) Is it possible to stack?ii) Cooling time??iii) Lifetime???iv) positron spin dynamics
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Which device for which cross section?
-12 -10 -8 -6 -4 -2 0
4
6
8
10
12
14
16Current for
p~1hour
Limit for stable operation of Antiproton storage ring
Toroidal storage ring (Stellatron) with electron cooling and stacking (????)
Strorage ring with pulsed injection(polarized electrons)
d.c.-source with online isotope production
Michigan sourcelo
g(f
lip c
ross
se
ctio
n)
[ba
rn]
log (Positron current) [A]
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Summary
• e+/pbar spin exchange cross sections could provide a (pbar)-loss free polarization mechanism
• Theoretical and experimental investigations for the cross section are underway and will probably lead to conclusive results this year
• Compact polarized positron sources with present day technolgy would yield 1 hour of polarisation time if the cross section is ~1010barn, (106 Barn with advanced technolgy??)
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Laser-Plasma-accelerator*
*W.P. Leemans et al: Nature physics, 2, 696 (2006)
3T-Laser:1.5J,40fs, 40TWdfok=50ma0=4.8reprate:1Hz
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e/-collider
*H Schwoerer et al. PhysRev.Lett., 96, 014802 (2006)
using part of the drive beamfor compton backscattering!
sub-picosecond duration circularely polarized gamma beam may be possible,thus increasing long. brightness by two orders of magnitude
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Laser-Plasma-accelerator*
*W.P. Leemans et al: Nature physics, 2, 696 (2006)
Electronen-Puls:1GeV,30pC, E/E=0.05Peak current 10kA! E*T]~0.1MeV*ps [x*]~10nm*rad
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• Pocket accelerators may provide efficient
source for polarized gamma radiation • at small size and investment/running cost
(compared to 1GeV high charge storage ring)• Potential for far higher luminosity could result in
2 orders of magnitude increase of bunch charge. (3*10^5 /pulse in storage ring acceptance)
• but: technology not (yet) well established.
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Once established, an e+ source operates like an e- source…..
Figure from van House et al. (1984)Beam energy: 500eV
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Intensity Limit of d.c. source?
Commercial PET-Isotope production:Proton cyclotron 20 MeV, 14N(p,)11C:Yield: 0.8*1010Bq/A.
Isotope Emax
[MeV]T1/2 Amax
[Bq/mg]REM
22-Na 0.5 2.6 a 2*1011 Van House: 2*1010
64-Cu 0.6 12.7h 1.4*1014 Highest activity:1015
18-F 0.6 109.7m 3.3*1015 PET
11-C 1.0 20.38m 3.1*1016 PET
15-0 1.7 2.03m 2.2*1017
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P2I-optimization
‚Optimum‘ positron source: Carbon-11 (E0=1MeV).Higher Polarization, far higher activity
also from van Houseet al.
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Expected d.c.-source parameters
Online C-11 production with Commercial superconducting Linac*: 1.2 mA, 20MeV 1013 Bq source activity Expected Efficiency increase: factor 2compared to 1980-s experiment
Current: 5*109 e+/sPolarization: 0.7Energy width: <0.1eVNormalized beam emittance 1 mm mrad
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e+-Storage ring option
1. Profit from enhanced Beam current due to revolution frequency.
2. Conventional AG-storage ring offers beam lifetime of several seconds @1MeV
3. longitudinal spin stabilization with -rotating solenoid seems feasible.
4. Space charge limit 10mA.5. Aim at >3*105 stored particles (1
Mikroamp i.e 3 orders of mag. w.r.t. d.c. source)
6. Task: Produce 3*105 pol e+ in acceptance of 5keV*ns.
Antip ro to n b e a m in sto ra g e ring
Sp in tra nsfe r re g io n
C irc um fe re nc e ~ 14m (f = 21 M hz)re v
Kic ke r
Po la rize d e so urc e+So le no id fo r lo ng .
Sp in sta b iliza tio n
Possibility of antiproton polarization by Spin transfer
32
General Idea:
ee
As for the ILC sources…..
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P2I-optimization
‚Optimum‘ positron source: Carbon-11 (E0=1MeV).Higher Polarization, far higher activity
also from van Houseet al.