transverse echo measurements in rhic -...
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1
Transverse echo measurements in RHIC
Wolfram Fischer
COOL 05, Eagle Ridge, Galena, Illinois19 September 2005
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Wolfram Fischer 2
Contents
1. Motivation2. Experiments at RHIC3. Simulations
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Wolfram Fischer 3
RHIC overview
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Wolfram Fischer 4
Luminosity lifetime of colliding Au79+ beams
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Wolfram Fischer 5
Motivation
• Luminosity lifetime for heavy ions dominated by IBS– Effort to implement stochastic cooling
here: M. Brennan, M. Blaskiewicz– RHIC II upgrade based on e-cooling
here: I. Ben-Zvi, A. Fedotov, G. Wang• Main emittance growth mechanism
working against cooling is IBS
→ Good knowledge of IBS growth rates needed to predict cooling times and equilibrium beam sizes
→ Cooling times of order 1 hour, cannot afford error larger than about factor 2
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Wolfram Fischer 6
Motivation
• IBS growth rate measurements usually done by observing the free expansion of bunches– Must be on time scale of interest [15min at injection, hrs at store]
– Need precise emittance measurement [not easy transversely]
• Echo measurements are– Much faster (~1000 turns), allow parameter scans– Potentially very sensitive– Do not rely on precise emittance measurement
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Wolfram Fischer 7
Transverse echoes
• Echoes well known in plasma physics
• Sensitive method to measure diffusion rates
• Theoretical accelerator papers byStupakov, Kauffmann (SSC)
• Longitudinal echos observed at– FNAL AA [Spenzouris, Colestock et al.]
– CERN SPS [Brüning et al.]
– BNL AGS [Kewisch, Brennan]
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Wolfram Fischer 8
Transverse echoes – phase space simulation
dipole kick filamentation
quadrupole kick echo• 1-turn quadrupolekick is difficult
• echo-like signalwas also observedwith 2 dipole kicks of different strength(F. Ruggiero, SPS)
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Wolfram Fischer 9
Transverse echoes – dipole moment simulation
[W.Fischer, B. Parker, O. Brüning, “Transverse echos in RHIC”, proceedings of the US-LHC Collaboration Meeting: Accelerator Physics Experiments for Future Hadron Colliders, BNL (2000).]
no quadrupole kick with quadrupole kick
echo amplitude reducedby diffusion processes
Amax
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Wolfram Fischer 10
Transverse echoes – echo amplitude formulae
• Approximate echo signal for one-turn quadrupole kick,small dipole kick, constants diffusion coefficient D0(Stupakov, PAC97 and Handbook)
• ηmax echo amplitude, a dipole kick, • Q=β/f at quad• τd=T0/4πµ decoherence time, T0 rev. time, ω0=2π/ T0
• τ time between dipole and quadrupole kick• µ detuning (∆Q at 1σ amplitude), ε distribution rms• D0 diffusion coefficient
ετωµτ
τη
3/81 320
20
max
DQ
aA
decho +
==
→ not applicable for RHIC experiments (due to parameter range)
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Wolfram Fischer 11
Pulsed quadrupole in RHIC
Air core magnet
(Tevatron slow extraction)
Length l 1.5 m
Transfer B/I 3.6 T/kA
Inductance L 105 µH
Current I 50 A
Voltage U 2 kV
Rise and fall time 13 µs (1 turn)
Parameter set is for a quadrupole
strength of k = 0.002/m (f = 500m).
[W. Fischer, A. Jain, D. Trbojevic, “The AC quadrupole in RHIC”, BNL RHIC/AP/165 (1999).O. Dressler, “Quadrupole kicker for RHIC”, BNL C-A/AP/60 (2001), J. Addessi, J. Piacentino, D. Warburton]
PFN
HV PS
Pulsed quadrupole
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Wolfram Fischer 12
RHIC transverse echoes (1)
First RHIC echoes
• Au79+ at injection• single bunch • dipole kick by injecting with angle
• 1-turn quad kick
[W. Fischer, R. Tomas, T. Satogata, PAC05]
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Wolfram Fischer 13
RHIC transverse echoes (2)
Can observe echoes only
• With dipole kick of a few σ
• Nonlinear detuning an order of magnitude larger than natural one
• Quadrupole kick times no larger than a few 100 turns
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Wolfram Fischer 14
RHIC transverse echoes (3)
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Wolfram Fischer 15
RHIC transverse echoes (4)
Scan of nonlinear detuning µ (octupoles)
- no echo without detuning, no echo with large detuning- very weak proton echoes (unexpected)
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Wolfram Fischer 16
RHIC transverse echoes (5)
Scan of quadrupole kick time τ
- no echo small τ, no echo with large τ- very weak proton echoes (unexpected)
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Wolfram Fischer 17
RHIC transverse echoes (6)
Scan of bunch intensity Nb (increasing diffusion from IBS)
- echo decreases with increasing bunch intensity (like IBS)- no proton data over sufficiently large range of Nb
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Wolfram Fischer 18
Simulations (1)
- only 1D- linear transfer matrixes- octupoles to adjust µ- typically 10000 particles- diffusion introduced through random kicksfrom Gaussian distribution(adjustable width, constantfor all amplitudes)
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Wolfram Fischer 19
Simulations (2)
Can find diffusion coefficient in simulation that approximately reproduces detuning scan for gold ions
Particles trapped in islands
2 orders ofmagnitude
in D0
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Wolfram Fischer 20
Simulation (3)
Simulation can reproduce experimental main features of experimental quadrupole kick time scan
Particles trapped in islands
2 orders ofmagnitude
in D0
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Wolfram Fischer 21
Simulation (4)
- Can find proportionality coefficient D0/Nb so that simulationfits experimental intensity dependency (→ extracts measured D0)
- Fitted D0 corresponds to emittance growth time of about 100 h,consistent with free expansion measurements (not very accurate)
Expect IBS growth rates for Cu about factor 2 smaller than those for Au
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Wolfram Fischer 22
Summary – Transverse Echoes in RHIC
• Transverse echoes observed in RHIC with Au79+, Cu29+, p+
– Dipole kick with injection under angle– Air core quadrupole provides 1-turn kick
• Diffusion with p+ stronger than with heavier ions (unexpected)• Observed intensity dependent echoes with Au79+, Cu29+,
→ were fitted to simulation results to extract diffusion rates