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Fourier Series Pulse Compression Damping Ring Kicker: another Progress Report

Fourier Series Pulse Compression Damping Ring Kicker: another Progress Report. George Gollin University of Illinois at Urbana-Champaign. Dog bone (TESLA TDR) kicker specs: impulse: 100 G-m (3 MeV/ c ) ± 0.07 G-m (2 keV/ c ) residual (off) impulse: 0 ± 0.07 G-m (2 keV/ c )

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Fourier Series Pulse Compression Damping Ring Kicker: another Progress Report

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  1. Fourier Series Pulse Compression Damping Ring Kicker:another Progress Report George Gollin University of Illinois at Urbana-Champaign George Gollin, Damping ring kicker report, March 9, 2005

  2. Dog bone (TESLA TDR) kicker specs: • impulse: 100 G-m (3 MeV/c) ± 0.07 G-m (2 keV/c) • residual (off) impulse: 0± 0.07 G-m (2 keV/c) • rise/fall time: < 20 ns • Perhaps larger (but less precise) impulse at injection, smaller (but more precise) impulse at extraction will be desirable. • Small ring kicker rise, fall times can be asymmetric: • leading edge < 6 ns, trailing edge < 60 ns The specs George Gollin, Damping ring kicker report, March 9, 2005

  3. Instead of a pulsed kicker, construct a kicking pulse from a sum of its Fourier components. Combine this with a pulse compression system to drive a small number of low-Q cavities. Illinois, Fermilab, Cornell are involved. Fourier series pulse compression kicker

  4. Fermilab Tug Arkan Euvgene Borissov Harry Carter Brian Chase David Finley Chris Jensen Timergali Khabiboulline George Krafczyk Shekhar Mishra François Ostiguy Ralph Pasquinelli Phillipe Piot John Reid Vladimir Shiltsev Nikolay Solyak Ding Sun This project is part of the US university-based Linear Collider R&D effort (LCRD/UCLC) Participants Cornell Gerry Dugan Joe Rogers Univ. Illinois Joe Calvey Michael Davidsaver Justin Phillips George Gollin Mike Haney Jeremy Williams

  5. Fermilab/Illinois activities • Initial studies: use Fermilab A0 photoinjector beam (16 MeV e-) for studies: • concept and design studies of FSPC kicker • build a fast, simple strip line kicker • use the stripline kicker to study the timing/stability properties of the A0 beam • build a single-module pulse compression kicker • study its behavior at A0 • perform more detailed studies in a higher energy, low emittance beam (ATF??) George Gollin, Damping ring kicker report, March 9, 2005

  6. Right now: simulations and RF engineering discussions…

  7. …and writing it up so it is clearly described… George Gollin, Damping ring kicker report, March 9, 2005

  8. Start with a simple kicker whose properties are calculable and can be measured independently of its effects on the A0 electron beam. Most important: how well can we measure a device’s amplitude and timing stability with the A0 beam? …and building a stripline kicker. Fermilab just finished building this. Install next month (April, 2005). George Gollin, Damping ring kicker report, March 9, 2005

  9. 16 MeV electron beam, good spot size, emittance. EOI submitted to A0 group last spring. Space in beamline will be available ~January 2005 Test it in the FNAL A0 photoinjector beam George Gollin, Damping ring kicker report, March 9, 2005

  10. Performance modeling studies • Functional units in the system, downstream to upstream: • RF cavity, Q = 25 • Waveguide • RF amplifier • Arbitrary function generator • Modeling strategy is to study the consequences of: • drifts in parameter values (e.g. Q of RF cavity) • noise in RF power amplifier output signal • nonlinearities: harmonic and intermodulation distortion George Gollin, Damping ring kicker report, March 9, 2005

  11. Parameter Symbol Value Main linac bunch frequency fL (wL ≡ 2p fL) 3 MHz Damping ring bunch frequency fDR (wDR ≡ 2p fDR) 180 MHz RF structure center frequency fRF (wRF ≡ 2p fRF) 1845 MHz RF structure Q Q 25 Waveguide cutoff frequency fcutoff 1300 MHz Desired on field integral A(0) (100 ± .07) Gauss-meters Desired off field integral A(t) (0 ± .07) Gauss-meters fDR / fL N 60 fRF / fDR G 10.25 fRF / fL GN 615 Bunch length dB or tB ±6 mm ~ ±20 ps Karma ☺ Impeccable Parameters in our studies Nothing has been optimized yet! George Gollin, Damping ring kicker report, March 9, 2005

  12. RF cavity • Q = 25 • center frequency 1845 MHz

  13. RF cavity Q error • Kick error caused by deviations in Q for the center, head, and tail of the kicked and first two unkicked bunches. Full vertical scale corresponds to 0.07 Gauss-meters (2.1 keV/c). George Gollin, Damping ring kicker report, March 9, 2005

  14. RF cavity center-frequency error • Kick error as a function of cavity center frequency error for kicked, first unkicked, and second unkicked bunches . George Gollin, Damping ring kicker report, March 9, 2005

  15. Waveguide: 80 meters long for the time being • 80 meters long • 1300 MHz cutoff

  16. Waveguide compresses pulse • Pulse compression! • Maximum amplitudes: • entering ~0.016 • exiting ~0.1

  17. Waveguide length error • Two contributions to problems: • change in flight time down the waveguide • relative phases of Fourier components are misaligned • #1 dominates. Differences between delivered kicks and an ideal impulse for waveguides that are 5 mm, 10 mm, 15 mm, 20 mm, and 25 mm too long. The peaks in the kicks have been shifted in time to align with the peak in the ideal impulse that is centered at t = 0. In addition, the delivered kicks have been rescaled to have the same magnitude as the ideal impulse. George Gollin, Damping ring kicker report, March 9, 2005

  18. Waveguide cutoff frequency error Correcting for time misalignment and change in overall pulse size helps considerably. Effects of cutoff frequency errors. The curves represent the difference between delivered and ideal impulses as functions of time after aligning the time of the peaks and rescaling the peak amplitudes. Full scale in the plot is 100 ps. Nominal fcutoff is 1.3 GHz. Errors in cutoff frequency for individual curves are indicated on the plot. George Gollin, Damping ring kicker report, March 9, 2005

  19. Amplifier gain error For now, look at a linearly increasing error as a function of frequency… Effects of an amplifier gain error that grows linearly with frequency. The curves represent the difference between delivered and ideal impulses as functions of time. The time region in the plot is centered on the arrival time of the kicked bunch. George Gollin, Damping ring kicker report, March 9, 2005

  20. Use a linearly increasing error as a function of frequency here too. Amplifier phase error Effects of an amplifier phase error that grows linearly with frequency. The curves represent the difference between delivered and ideal impulses as functions of time. The time region in the plot is centered on the arrival time of the kicked bunch. Full (horizontal) scale is 100 ps. The impulse functions have been shifted in time to align the kicking peaks at t = 0 and rescaled to agree in amplitude with the nominal kick George Gollin, Damping ring kicker report, March 9, 2005

  21. Model as flat in frequency, from 300 MHz to 6 GHz for now. Cavity is insensitive to frequencies far from center frequency… 10-4 GHz-1/2 Amplifier noise… George Gollin, Damping ring kicker report, March 9, 2005

  22. Generate in 300 kHz frequency bins, random phases. More work is needed… …amplifier noise George Gollin, Damping ring kicker report, March 9, 2005

  23. Nonlinear effects: harmonic and intermodulation distortion Initial harmonic distortion studies are done. Now working on intermodulation distortion simulation. George Gollin, Damping ring kicker report, March 9, 2005

  24. Harmonic distortion George Gollin, Damping ring kicker report, March 9, 2005

  25. Intermodulation distortion Intermodulation distortion: third-order effects are most likely to be the most important. Under way… George Gollin, Damping ring kicker report, March 9, 2005

  26. Building a stripline kicker

  27. Looking inside the kicker

  28. Baking the kicker electrodes Kicker is now assembled, vacuum tested, “high-potted.” Installation in A0: mid-April.

  29. Measuring electrode positions George Gollin, Damping ring kicker report, March 9, 2005

  30. Machineable ceramic supports

  31. UIUC students in A0

  32. …but we’ve started working on analysis tools. Our plan is to generate simple Monte Carlo data to test tools before we have real data. We bought a new computer: No data yet…

  33. We started looking at (old) straight-through A0 data

  34. Start with a Fermilab linac chopper HV pulser: ±750 V. Chris Jensen and colleagues just finished it. HV pulsers

  35. FID pulser • Gerry Dugan is ordering a FID pulser: • Maximum output into 50 Ohm: ±1 kV • Amplitude stability in burst mode 0.3 – 0.5% • Pre- and after-pulses 0.3 – 0.5% • Rise time 10-90% of amplitude 0.6 – 0.7 ns • Pulse duration at 90% of Umax 2 – 2.5 ns • Fall time 90-10% of amplitude 1 – 1.5 ns • Maximum PRF in burst mode 3 MHz • Maximum PRF in continuous mode 15 kHz • Timing jitter, both output pulses vs. trigger 20 ps, max • Power 110/220VAC, 50/60 Hz

  36. Design, then build one module using existing components. • Fermilab RF group is involved • UIUC HEP electronics design group’s chief is too. • So we’re making progress. • Goals: • install strip line kicker in A0 during April, 2005 • understand A0 by summer, 2005 • investigate small pulse compression system during summer, 2005 UIUC/FNAL, longer term plans George Gollin, Damping ring kicker report, March 9, 2005

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