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

12. September 2011 1.537

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