. . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . .. . . . . . . Fourier Series Pulse Compression Damping Ring Kicker . . . .. . . . . . . . . . . . . . . . . . . . . George Gollin University of Illinois at Urbana-Champaign and Fermi National Accelerator Laboratory . . . . ..
Download ReportTranscript . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . .. . . . . . . Fourier Series Pulse Compression Damping Ring Kicker . . . .. . . . . . . . . . . . . . . . . . . . . George Gollin University of Illinois at Urbana-Champaign and Fermi National Accelerator Laboratory . . . . ..
. . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . .. . . . . . . Fourier Series Pulse Compression Damping Ring Kicker . . . .. . . . . . . . . . . . . . . . . . . . . George Gollin University of Illinois at Urbana-Champaign and Fermi National Accelerator Laboratory . . . . .. . . .. . George Gollin, Damping ring kickers, KEK ILC, November 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 1 . . . . . . . .. . . . . . . . . . . . . . . . . . .. . . . . . . . .. . . . . .. . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . .. . . . . . . . . .. . . .. . . . . . . . . . . . . . . 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 . . . . .. . . .. . George Gollin, Damping ring kickers, KEK ILC, November 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 2 . . . . . . . . . . . . . . . . . . . . . Dog bone (TESLA TDR) kicker .specs: . . . . . . . . . . . . . . . G-m (2 keV/c) • impulse: 100 G-m (3 MeV/c) ± 0.07 . . . . . . . . . . . . • residual (off) impulse: 0 ± 0.07 G-m (2 .keV/c) . . . . • rise/fall time: < 20 ns . . . . . . . . . . . . . . . .. . . . . . . . . . . . .. The specs . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . .. . . . . . . .. . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . .. Combine this. with a pulse compression system to drive a small number . . . of low-Q cavities. . . . Illinois, Fermilab, Cornell are involved. . .. . . . . .. . . .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 3 . . . . of its . .. . . . Instead of a. pulsed kicker, construct a kicking pulse... from a sum . . . . . . . . . . . . . . Fourier components. . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . Fourier series pulse compression kicker . . . . .. . . . . . . . . . . . . . . . Joe Rogers .... . .. . . . . .. . . . . . . . . . .. . . .. . . . .. . . . . . . Cornell University . . . . . . . .. .. . . . . . . . . . . . . . . . . . Brian Chase David Finley Chris Jensen George Krafczyk Shekhar Mishra François Ostiguy Ralph Pasquinelli Phillipe Piot John Reid Vladimir Shiltsev Nikolay Solyak Ding Sun… . . . . .. Guy Bresler Joe Calvey Michael Davidsaver Keri Dixon George Gollin Mike Haney Tom Junk Jeremy Williams . . Fermilab . . . . . . . . .. University of Illinois. . Physics P llinois . . 4 . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . US. university-based Linear . . . project is part of the This . .. . . . . . . . . . . . . .Collider R&D. effort (LCRD/UCLC) . . I . . . . . . .. . . . . . . . . . . . . . . Participants . .. . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . studies: use Fermilab A0 photoinjector beam (16 . MeV . . . . . electrons) .for studies: . .. . . . . . . . . . . . . .. . . 1. build a fast, simple strip line kicker 2. use the kicker to study the timing/stability properties of the A0 beam 3. build a single-module pulse compression kicker 4. study its behavior at A0 5. perform more detailed studies in a higher energy, low emittance beam (ATF??) . . . . .. . . .. . George Gollin, Damping ring kickers, KEK ILC, November 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 5 . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . .. . . . . . .. . . . . . .. . . . . . . Fermilab/Illinois activities . . . . . Initial . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . .... . .. . . . . .. . . . . . . . . .. . . . .. . . . . . . . . .. . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . .. . . . . . . . . I . . . . . . . . . .. . . . . . .. . . . . .. . . Physics P llinois . . . . . . . . . . . . . .. . . . . . . . . . .. . . . . . . . . 6 . . . .. . . Right now: simulations and RF. engineering discussions… . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . .. . . .... . .. . . . . .. . . . . . . . .. . . . . .. . . .. George Gollin, Damping ring kickers, KEK ILC, November 2004 . . .. . . . . . . . . 7 . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . .. . . . . .. . . Physics P llinois . . . . . . . . . . . . .. . . . . . . . . . I . . . . . . . …and writing it. up so it is. clearly described… . . . . .. . . . . . . . . . . . . .. .. . . . . . . . . . . . . . . . . . . . . . .. . . . .. . . . . . are calculable Start with. a. simple kicker whose properties and can . . . . . be. . . . . . . . . . . . its effects . . measured independently of on the A0 electron beam. . . . . . . . . . . . . . . . . . . . . . . . amplitude and Most important: how. well can we measure a device’s timing stability with the A0 beam? . .. . . .. . . . . . . . . . . . . . flanges beam pipe BPM beam pipe BPM BPM stainless steel pipe BPM conducting rods Fermilab is currently building this. Probably ready by January 2005. . . . . .. . . .. . George Gollin, Damping ring kickers, KEK ILC, November 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 8 . . . . . . . . . . . . . . . . . .. . . . . . . . …and building a stripline kicker. . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . .. . . . . . . . . . . last spring. . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . .. EOI submitted to A0 . . group . . . .. . . . . . . . . . . . . . . . . . . . . . . . Space in beamline will be available ~January 2005 . . . . .. . . .. . George Gollin, Damping ring kickers, KEK ILC, November 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 9 . . . . . . . . . . . . . .. . . . . . . . . . . . . . .. . . . . . . 16 MeV electron beam, good spot size,. emittance. . . . . . . Test it in the FNAL A0 photoinjector beam . .. . . . . . . . . . . . . .. . . . . . . .. . . . . . . . . . .. . . . . . . . . . . . . . . . involved . . . Fermilab RF group is . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . UIUC HEP electronics design group’s chief is too. So we’re making progress. Goals: • install strip line kicker in A0 by January, 2005 • understand A0 by spring, 2005 • investigate small pulse compression system by summer, 2005 . . . . .. . . .. . George Gollin, Damping ring kickers, KEK ILC, November 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 10 . . . . . . . . .. . . . . . . Design, then build one module components. . . .using existing . . . . . . . . . . . . . . . . .. . . . . . .. . . . . . . . . . . . . . . . . . UIUC/FNAL, longer term plans . . . . . . .. . . . . . . . . .