Impedance Database and Its Application to the APS Storage Ring Yong-Chul Chae Advanced Photon Source 2007 ILC Damping Rings Mini-Workshop, 18-20 December,

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Presentation transcript:

Impedance Database and Its Application to the APS Storage Ring Yong-Chul Chae Advanced Photon Source 2007 ILC Damping Rings Mini-Workshop, December, 2007 High-Energy Accelerator Research Organization, KEK, Tsukuba, Japan

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Outline Impedance Database (  z = 5 mm) Application: understanding observed instability –Longitudinal Microwave Instability –Horizontal Saw-Tooth Instability –Vertical TMCI Instability –Injection Process Impedance Database II (  z = 1 mm) –Improvement –Accumulation Limit Plan for the future APS Upgrade –Energy Recovery Linac

ILC Damping Rings Mini-Workshop at KEK, December 18-20, APS RF Cavity

ILC Damping Rings Mini-Workshop at KEK, December 18-20, D ABCI simulation APS RF Cavity: Wakefield Wakefield Bunch

ILC Damping Rings Mini-Workshop at KEK, December 18-20, D ABCI simulation APS RF Cavity: Wakepotential

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Mhz fundamental Broadband: short range including beam loading Narrowband: long range including beam loading HOMs APS RF Cavity: Impedance

ILC Damping Rings Mini-Workshop at KEK, December 18-20, W total = total wake-potential of the ring, N i = number of the element in the ring, W i = wake-potential of the element, a i = weight of the element. GOAL: Total Wake Potential Impedance Database

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Impedance Elements 2cm 1cm 4cm 153 mm 8 mm 

ILC Damping Rings Mini-Workshop at KEK, December 18-20, VERTICAL LONGITUDINAL HORIZONTAL Total Impedance of the APS Storage Ring

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Shifted Spectrum, H0(  ) Impedance, Zy Zeff=H0*Zy Tune Shift: Formula

ILC Damping Rings Mini-Workshop at KEK, December 18-20, APS Low Emittance Lattice

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Calculated Tune Slope = 2.2e-3/mA Measured Tune Slope = 2.4e-3/mA Tune Shift: Vertical

ILC Damping Rings Mini-Workshop at KEK, December 18-20, (Y.Chae, L.Emery, A.Lumpkin, J.Song, PAC’01) Longitudinal MW: Measurement  t vs. I  E vs. I

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Longitudinal MW: Measurement fs 4*fs 2.4 mA 6.7 mA 6.9 mA 16 mA Mosnier: 8 f r  t = 1 + m  f r =25 GHz,  t =40 ps  m = 7

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Bunch Length Oscillation Bunch Length/Energy Spread Longitudinal MW: Simulation

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Longitudinal MW: Simulation Bunch Length Bunch Center

ILC Damping Rings Mini-Workshop at KEK, December 18-20, What limits the single-bunch current? Accumulation Limit was 6-8 mA at low chromaticity at 5-7. Chromaticity was limited by sextupole strength until the pole tip was modified. Higher chromaticity (> 10) achieved with modified sextupoles. Accumulation Limit is 20 mA at high chromaticity at 10.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Vertical TMCI: Simulation Centroid Kick  y=1mm SpectrumVertical Beam Size 2 mm 3 mm 1.Well known decoherence behavior at low current 2.Mode coupling completes 3 mA 3.Beam size blow-up above mode coupling  Beam Loss due to 5-mm Insertion Device Chamber

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Gated Camera Images: I=1 mA, IK1=1 kV Turn-by-Turn Images Gated Camera and Kicker are synchronized Kick the beam; Capture single image; Wait for damping; Repeat

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Horizontal Beam Size: Low Current (1 mA) Measurement: BM Visible, IK1=1 kV, Simulation: ID, BBR-1,  x=2 mm Beam size normalized by the maximum for comparison

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Vertical Beam Size: High Current (5 mA) Measurement: ID x-ray pinhole, IK5=1 kV, Simulation: ID, BBR-1,  y=50  m Beam size normalized by the maximum for comparison

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Simulation of Injection Process Purpose is to improve the accumulation limit above 8 mA at low chromaticity setting –Injection by matched kicker bumps –Injection by mismatched kicker bumps (current) –Longitudinal injection (proposed)

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Injection by Mismatched Kicker Bump From Louis Emery (APS/OAG) 8mm

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Injected Beam Stored Beam x y Stored beam Injected beam  x (mm) 34  y (mm) 00.2  x (m) 3e-91.5e-7  y /  x (%) 310  x (m) 20  y (m) 33  s (mm)  p (%) Coordinates of Initial Beam at the center of ID straight Initial Condition of Beam Simulating Current Injection Scheme

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Injection Efficiency vs. Current Accumulation Limit Measured Accumulation Limit < 8 mA

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Significant amount of stored beam is lost during the injection process Reduce the Beam Loss  Reduce the Separation  Longitudinal Injection Injected Beam Stored Beam x y Initial Coordinates of Lost Beam

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Longitudinal Injection Scheme

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Injection Efficiency Improved in simulation ! Longitudinal Injection Current Injection Injection Efficiency vs. Current

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Prediction of Accumulation Limit: High Chromaticity Threshold current is 20 mA determined by simulation –Vertical beam size blow-up Simulation reproduced the accumulation limit at 20 mA observed in the APS storage ring

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Single Bunch: Prediction for the APS We can now predict the effect of small gap chambers.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, So far so good, but some problems to be fixed The impedance to produced good agreement was NOT true impedance BUT “Working Impedance” –We add imaginary Z/n=0.1  to the computed impedance –This is necessary to compensate missing impedance above GHz Bunch length oscillation of 5-ps amplitude had never been verified by streak camera measurement with 2- ps resolution. If the accumulation is limited by a vertical TMCI, why our injection efficiency is sensitive to the HORIZONTAL injection kicker setting in a high chromaticity operation?

ILC Damping Rings Mini-Workshop at KEK, December 18-20, So far so good, but problems to be fixed (2) 200 ps 20ps Phase space modulation is questionable.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Impedance Database II: Choice of Bunch Length The shorter, the better. But, computer resources are limited. We choose  z =1 mm –quasi-Green Function We purchased 60-node cluster equipped with 240 GB of memory We purchased GdfidL Remove “ad-hoc” modification made to IDB-1 by improving the impedance bandwidth Use short bunch to calculate wake potential!

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Impedance Database II: Results Bandwidth increased from 40 to 200 GHz! 200 GHz 500 GHz 50 GHz W z (V/pC) | FFT(W z )|

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Bunch Length Measurement Simulation results was obtained by a raw impedance.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Energy Spread Measurement The difference is only 2% if we include 40 um resolution.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Phase space is smoothed The pronounced paw-like structure is smoothed. P=6500 P=7000 P=7500 P=8000

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Bunch Length Variation is reduced. The oscillation amplitude is about 2 ps close to the APS streak camera limit.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Accumulation Limit This is the first time we compare accumulation limit at different values of chromaticity.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Beam Loss Effect of amplitude dependent tune shirt changes beam-loss plane from vertical to horizontal plane. Vertical TMCI Horizontal TMCI

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Single Bunch Current of the Future APS Ring Add (%)Total (%)Current (mA) Note Reference *5-mm + 29*8-mm + Others Short pulse sector *3-cell + 2*9-cell (r=23.5 mm), T1+T2 8-mm gap Replacing S11 4*8-mm gap New addition 7-mm gap0.64 (2.18) Replacing 8mm 3.5 m long SC ID 6-mm gap1.71 (3.25) Replacing 8mm 5 m long S1

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Plan for the APS Upgrade We consider upgrading the current 3 rd generation storage ring to an Energy-Recovery-Linac based 4 th generation light source. –Need to compute the wake potential of 100-fs bunched beam passing through linac and all impedance elements We are developing a high-order 3D wake-potential program based on a spectral-element discontinuous Galerkin method –the wake potential of 9-cell TESLA cavity –the wake potential of undulator chambers with nonlinear transition (x, x^2, etc) We are developing a high-order 3D time-dependent PIC code in collaboration with Brown University –Initially we will simulate 1-m long structure: rf-gun –Eventually we will simulate 1-km long structure without any approximation: accelerator This is in the LDRD proposal with strong support from ANL’s petaflop computing.

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Summary Impedance Database was proved as a useful tool to investigate the single-bunch instability in the APS: –The APS storage ring –The 1-nm storage ring with smaller chamber –The APS storage ring with crab cavities for short x-ray pulse Found that 3D computation was essential because the APS storage ring’s chamber is smooth. Very short bunch in the ERL based APS Upgrade required to develop a new high-order 3D wake-potential code

ILC Damping Rings Mini-Workshop at KEK, December 18-20, Acknowledgement Taking Data M. Borland, L. Emery, K. Harkay, A. Lumpkin, N. Sereno, V. Sajaev, J. Song, C. Yao, B. Yang, APS Operators Computer Software/Hardware M. Borland, B. Soliday, Y. Wang, A. Xiao, W. Bruns (GdfidL) Drawings P. Choi, G. Goepner, L. Morris, E. Rossi, S. Sharma Support R. Gerig, K. Harkay, K. Kim, S. Milton Discussion S. Krinsky, B. Podobedov, J. Wang (NSLS) R. Nagaoka (SOLEIL), M. Blaskiewicz (BNL)