. . . . . . . . . . . . . .. . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . George Gollin University of Illinois at Urbana-Champaign and Fermi National Accelerator Laboratory . . . . ..
Download ReportTranscript . . . . . . . . . . . . . .. . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . George Gollin University of Illinois at Urbana-Champaign and Fermi National Accelerator Laboratory . . . . ..
. . . . . . . . . . . . . .. . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . George Gollin University of Illinois at Urbana-Champaign and Fermi National Accelerator Laboratory . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 1 . . . . . . . . . . . . .. . . . . . .. Damping ring kickers . . . . . . . . . . . . . . . .. .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . .. . . . . . . . • Current ideas • Opinions from the speaker • Illinois/Fermilab efforts • ILC-America + ILC-global near term goals . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 2 . . . . . . . .. . . . . . . . . . . . . . . . .. . . . • The specs . . . . . . . . . . . . .. . .. . . . . . . . . . . . . . . . . . . . . . •. The problem . . . . .. . . . . . . . .. Outline . . . . . . . . . . . . . . . . .. . . .. . . . . . . . .. . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Linac . beam (TESLA TDR): . . .. . . . . . . . . . . . . . . . 340 . (~. 300 kilometers) . • .2820 bunches, nsec spacing . . . . . . . . . . . . . • Cool an entire pulse in. the damping rings before linac injection . .. . . ILC damping ring beam: • 2820 bunches, closely spaced • Eject every nth bunch into linac (leave adjacent bunches undisturbed) • Minimum damping ring circumference depends on minimum realizable bunch spacing (kicker speed and instability issues) Kicker: • 20 ns kicker 17 km circumference (TESLA dog bone) • 6 ns kicker 6 km circumference (Fermilab small ring) . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 3 . . . . . . . . . . . . . . . . . .. . . . . . . . . . .. The problem . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . .. . . . . . . . in tackling There’s significant global interest the challenges posed . . . . . . . . . by the damping ring and kicker. . . . . . . . . . . . . . . . .. . We have already started an informal, global “conversation”: see Andy Wolski’s site at http://awolski.lbl.gov/ILCDR/. for a partial list of who has made contact. There are physicists from ANL, CERN, Cornell, Daresbury, DESY. Fermilab, Frascati, Harvard, Illinois, KEK, LBNL, Minnesota, SLAC, Tokyo so far. . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 4 . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . .. . . . .. . . . . . . . . . . . . . . . . . . . . . . . . What an.. interesting problem! . . . . . . . . .. . . . . . . . . . . . . . . . .. .. . . . . . . . . . .. . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . Extraction: • damping is finished, bunches are small (a few microns in diameter) ; • kicker must preserve beam emittance for still-orbiting bunches as well as the kicked bunch. Performance demands on kicker are different for injection/extraction. Should we consider separate designs for injection and extraction? . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 5 . . . . . . . Injection: . . . . .. . . . . . . . . . . . . . . . . • already-orbiting damped appreciably, have large . . bunches have not . . . . . . . . . . . . . . transverse sizes. (~2 cm); . . . . . . . • kicker must inject new bunches into damping ring .acceptance without . . losing already-orbiting bunches. . . . . . . . . . . . .. . . . . . . . . . . . What we have to work with . . . . . . .. . . . . . . . . . . . . .. . . . .. . . . . . . . . . .. . . .. . . . . . . . . . . . . . . . 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 . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 6 . . . . . . . . . . . . . . . part, .. . . .. . . .space Kicker .specs depend, in on beam dynamics: phase volume . . . . . . .. . . . be well separated . . occupied by. . a just-kicked bunch must from that of . . . . . . . . . . . . . . . an .unkicked bunch. . . . . . . . . . . . . . . . . . . The specs . . . . . . . . . . . . . . . . . . . . . . .. . . .. . . . . .. . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . line . Fast switches dump high voltage pulses into a series of strip . . . . .. . . . . . . . . . structures. . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . Electromagnetic pulse applies transverse kick to. one bunch, but .is . . . . . absorbed in .a load in each strip line module before next bunch arrives. . . • switch speed, on-resistance, and stability are concerns • adequate precision of strip line termination is challenging . . . . . . . • TESLA and SLAC are thinking about this . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 7 . . . The ideas (1): strip line kicker. modules . . . . .. . . . . . . . . . . . . . . . . . . . . . . . .. . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Demands on kicker are less. severe: it. only sees every 4. th bunch. . . . . . . . . . . . . . .. . . . multiple paths. . . . . . . . . . . . .. . . . . . . . along . . . . . . . .. . . Separate the .beam so . that it travels . . . . .. . . . . . . . .. . . . . . The system needs to be studied in detail: how to do it, what happens . . . when it is installed in a damping ring. . .. . . Cornell, Frascati are thinking along these lines. . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 8 . . The ideas (2): longitudinal kick +. dispersion . . . . . . . . . . . . . . . . . . . . . . pulse. from a sum of its . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . .. . . . . . . . . . . . . Most interesting (to me) .idea now: combine this with a pulse . . . . . compression system to. drive a small number of low-Q . cavities. • what are stability requirements on RF components? • how robust to bunch arrival time errors can the system be made? . . . . . . . . . . Illinois, Fermilab, Cornell are involved. . .. . . . . .. . . .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 9 . . . . . . . . .. . . . . .. . . . .. . . . kicking . . . . . . . . . .. . . . . . . . . . . . . . . . . The ideas (3): Fourier engineering . . Instead of a pulsed kicker, construct a . .. . . . . . . Fourier components. . . . . . . .. . . . . . . . . . . . . . .. . . . . . . . . .. . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . Damping ring architecture (bunch timing structure, injection/extraction . . . optics, etc.) is strongly tied to details of the kicker. . . . A fast pulsed kicker might be simplest to operate BUT switch speed and stability are challenging issues. Significant proof of the feasibility of at least one design is needed before a choice of damping ring design (big ring vs. small ring) will be possible. . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 10 . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . potential to be. a “show-stopper.” The kicker has the . . . . . . . . . . . . . .. .. . . . . . . . . . . .. . . .. . . . . . . The speaker’s opinions .(1) . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . Perhaps these features should be included in all damping ring designs? There are three distinct stages in damping process: • injection and assembly of bunch trains • damping • disassembly of bunch trains and extraction Beam is very different in each of these stages. Should there be distinct subsystems (including different kickers) for each of them? . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 11 . . . . . Fermilab small ring studies . . . . .. . . . . . . . . . . . . . . . . . . ~60 . • damping ring. bunch trains with ns inter-train gaps . . . . . . . . . . . . . . • long straight section to. allow installation of as-yet unspecified . kicker . .. . . . . . . . . incorporate: . . .. . . .. .. . . . . . . . . . . . . . The speaker’s opinions .(2) . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . .. . . . . .. . . . .. . . . . .. . . . . . .. . . . . . . . . Large acceptance injection ring: . . . . . .. . . . . . . . . . . . . . . . . . . . . . • (340 . . . . . – 6) = 334 ns circumference . . . . . . . . . • assemble .a single bunch train by injecting successive bunches. into . .. . . this ring at the tail of the train already orbiting the. injection ring • transfer entire bunch train into the damping ring in one orbit . . . . . . . . . . . . . . . Large acceptance damping ring (6 ns bunch spacing) Small acceptance extraction ring: • (340 + 6) = 346 ns circumference • transfer one entire bunch train from the damping ring • extract by kicking the last bunch in the train on successive orbits . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 12 . . .. . . . Separating injection, damping, extraction functions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . .. . .. . . . . . . . .. . . . . . . . . . . . . . . .... . .. . . . . .. . . . . . . . . . . . . . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . .. . . . . . . . . . I . .. . Physics P llinois . . . . . . . . . . . Injection and extraction rings differ in circumference by two bunch . . . . . . . . . . . . . . . train. spacings to allow injection/extraction to/from tail of bunch . . . . . . . . . . . . . . . . .. . . . . . . . .. . .. . . . . . . . . . . . 13 . . .. . . . Separating injection, damping, extraction functions . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . . . . 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, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 14 . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . .. . . . . . .. . . . . . .. . . . . . . Fermilab/Illinois activities . . . . . Initial . . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . .. . . . . . .. . . . . last spring. . . . . . . . . . . . . Space in beamline will be available ~January 2005 . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 15 . . . . . . . . . EOI submitted to A0 . . group . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . 16 MeV electron beam, good spot size,. emittance. . . . . . . . . . . . . . . .. . . .. . . .. . . . . . . . . . . A0 photoinjector beam . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . .. . . . .. . . . . . 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 designing this. Probably ready by January 2005. . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 16 . . . . . . . . . . . . . . . . .. .. . . . . . . . . . . . . Simple kicker for initial tests . . . . . . . . .. . . . . . . . . . . . . . . . . . . .. . . . . . . . . . .. . . . . . . involved . . . . . . . . . . . Fermilab RF group is . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . UIUC HEP electronics design group’s chief is too. So we’re starting to make progress. Goals: • install strip line kicker in A0 by January, 2005 • understand A0 by spring, 2005 • install small pulse compression kicker at A0 by summer, 2005 . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 17 . . . . . . . . .. . . . . . . Design, then build one module components. . . .using existing . . . . . . . . . . . . . . . . .. . . . . . .. . . . . . . . . . . . . . . . . . UIUC/FNAL, longer term plans . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . . . .. . . .. . . . . . . .. . . . . . . . . . .. . . . . . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . .. • pre-KEK:. discuss tentative plans for kicker R&D with our . . . . colleagues in America, Asia, and Europe to have a sense of who would like to do what. . . . . • at KEK: rough-out an R&D plan aimed at choosing a kicker technology in ~2 years • at Snowmass (August, 2005): kicker workshop with international participation to assess how well we’ve gotten started, and what we have learned . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 18 . . . . . . . . . .. . . . . . . . . . . Possible goals. and timelines: . . . . . ILC-America + ILC-global near-term goals . .. . . . . . . . . . . . . . . . . . . . . . . . .. . . . . . . . . . . .. . . . . . . . The. kicker and damping ring scare. .the daylights out of me.. . . . . . . . . . . . . . . . . . . . . . . . .. . . We must build one and make it work before the ILC . main linac is . . completed. . . . . More information: • Studies Pertaining to a Small Damping Ring for the International Linear Collider, FERMILAB-TM-2272-AD-TD • ILC Damping Rings web site: http://awolski.lbl.gov/ILCDR/ . . . . .. . . .. . George Gollin, Damping ring kickers, SLAC ILC-America, October 2004 .. . . . . . I Physics P llinois .... . .. . . . . .. . . . . . 19 . . . . . . . .. . . . . . . . . . . . . . . . .. . . . . .. . . . . . . . .. . . . . . . . . End notes . . . . . . . . . . . .. . . . . . . . .. . . . . . . . . . .