Transcript Folie 1
Beam Cooling at HESR in the FAIR Project
12 th September 2011 Dieter Prasuhn
HESR Consortium ICPE-CA, Bukarest, Rumania
Rumania 12. September 2011 Dieter Prasuhn 2
Outline
Design requirements for the HESR
Requirements for Cooling
p-bar injection and accumulation
Summary
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Modes of Operation with PANDA
Experiment Mode
Target rms-emittance Momentum range Intensity Luminosity rms-momentum resolution 12. September 2011
High Resolution Mode High Luminosity Mode
Hydrogen Pellet target with 4*10 15 cm -2 1 mm mrad 1.5 – 8.9 GeV/c 1.5 – 15.0 GeV/c 1*10 10 1*10 11 2*10 31 cm -2 s -1 2*10 32 cm -2 s -1 5*10 -5 1*10 -4 Dieter Prasuhn 4
Basic Data of HESR
Kicker Electron cooler Stochastic cooling vert.
hor.
long.
PU Circumference 574 m Momentum (energy) range
PANDA
1.5 to 15 GeV/c (0.8-14.1 GeV) Injection of (anti-)protons from CR / RESR at 3.8 GeV/c Maximum dipole field: 1.7 T p_bar injection Dipole field at injection: 0.4 T Dipole field ramp: 0.025 T/s Acceleration rate 0.2 (GeV/c)/s 5 12. September 2011 Dieter Prasuhn
Cooling requirements for HESR
Internal target (d=4*10 15 cm -2 ): • • •
Emittance growth Mean energy loss Small momentum spread (10 -5 )
Accumulation of p-bars in the HESR 12. September 2011 Dieter Prasuhn 6
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Antiproton Chain (Modularised Start Version)
p-linac SIS18 UNILAC HESR SIS100
•
acceleration in p-linac to 70 MeV
•
multiturn injection into SIS18, acceleration to 4 GeV
•
transfer of 4 SIS pulses to SIS100
•
acceleration to 29 GeV and extraction of single bunch pbar target/ separator
• •
antiproton target and separator for 3 GeV antiprotons collection and pre-cooling of 10 in the Collector Ring CR 8 p-bars CR
• •
transfer of 10 8 p-bars at 3 GeV to HESR accumulation and storage of antiprotons in the HESR
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p-bar injection and accumulation in the HESR
The p-bar accumulation without RESR
• • • • 10 8 p-bars collected in the CR 10 s cooling time in CR Transfer of 10 8 p-bars to HESR • In parallel: Cooling of 10 8 Cooling of 10 8 p-bars in CR p-bars in HESR • • ⇒ Transfer of 2 nd CR-stack into HESR 100 times repetition of that procedure Accumulation of 10 10 p-bars in HESR in 1000 s Acceleration, cooling, experiment 10 12. September 2011 Dieter Prasuhn
The accumulation process in HESR
12. September 2011 Simulations by H. Stockhorst and T. Katayama Dieter Prasuhn 11
Proof of principle experiment in the ESR
Properties of the ESR
circumference g transition beam 108 2.37
ARGON mass number charge state 40 18 kinetic energy b g revolution period D p/p injected 400 0.71
1.43
507 1.5*10 -3 emittances hor./vert. 1 12. September 2011 Dieter Prasuhn m MeV/u ns mm mrad 13
Experimental study of accumulation in ESR with barrier bucket and stoch. cooling
Collaboration: FZJ, GSI, Tokyo, JINR, CERN 12. September 2011 Dieter Prasuhn 14
Measured intensity increase by accumulation in the ESR
0.35
0.3
0.25
Fixed Barrier 0.2
• • • 0.15
Injection every 13 s 0.1
Accumulation over 500 s Saturation with 6*10 7 Ar ions 0.05
0 -200 -100 0 100 200 Accumulation Time [s] 300 400 12. September 2011 Dieter Prasuhn 15
Results
• • • • The idea of injection into the barrier bucket works Stochastic cooling is necessary to cool injected ions into the stable area Electron supports the efficiency by cooling oscillations by kicker ringing Simulation results agree with the experimental data 12. September 2011 Dieter Prasuhn 16
Question of the experimentalists:
Accumulation in HESR to more than 10
10
p_bars ?
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Cooling time for different intensities 60
• The beam from CR with D p/p = 5*10 -4 has to be cooled to 2.5*10 -4 • Due to longer cooling times than 10 s the efficiency decreases
50 40 30 N = 10 11 , 108 dB N = 5 x 10 10 , 114 dB N = 10 10 , 128 dB
• 5*10 10 p_bars seem to be possible within 5000 s accumulation time
20 10 0 0 N = 10 8 , 130 dB 5 10 Time [s] 15 20
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Study of internal Target effects
Operation of COSY Design and Construction of HESR
• Circumference: 184 m • Maximum momentum: 3.7 GeV/c (B r =12 Tm) • (un-)pol. Protons and Deuterons • Electron and stochastic cooling • Circumference: 574 m • Maximum momentum: 15 GeV/c (B r =50 Tm) • (un-)pol. Anti-protons • stochastic (and electron) cooling
COSY HESR
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HESR Prototyping and Tests with COSY Pellet Target WASA Barrier Bucket Cavity Stochastic Cooling
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Example: Beam Cooling with WASA Pellet Target
6 10 -7 5 10 -7 4 10 -7
d) a) Injected beam b) Beam heated by target c) + stochastic cooling d) + barrier bucket
3 10 -7 2 10 -7
c) a) b)
1 10 -7 0 1.5368
1.5369
1.5372
1.5373
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f [GHz] 1.5371
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Parameters for the HESR stochastic cooler: Momentum range (antiprotons): 1.5 - 15 GeV/c Band width: 2 - 4 GHz, high sensitivity Longitudinal cooling: Notch-Filter, ToF Aperture of couplers: 89 mm Octagonal Slot-Coupler Octagonal Printed-Loop Coupler
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Stochastic cooling pickup (prototype) installed in COSY
Same sensitivity as movable l /4 structures 12. September 2011 Dieter Prasuhn 24
HESR Prototyping and Tests with COSY Pellet Target WASA Barrier Bucket Cavity Stochastic Cooling
12. September 2011 Poster by Rolf Stassen Dieter Prasuhn 25
Next step in COSY: Electron cooling up to maximum momentum
Electron Cooling: Development Steps
HESR: 4.5 MeV
Upgradeable to 8 MeV COSY: from 0.1 MeV to 2 MeV Talk by J. Dietrich
Technological challenge
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Summary
• • • Strong cooling is essential for HESR Stochastic cooling is designed, prototype structures for 2-4 GHz tested Electron cooling in HESR will improve the experimental conditions and the accumulation efficiency • Tests will be performed at COSY with simultaneous electron and stochastic cooling in interaction with a thick internal target 28 12. September 2011 Dieter Prasuhn
Thank you for your attention 12. September 2011 Dieter Prasuhn 29