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US LHC Accelerator Research Program

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Presentation on theme: "US LHC Accelerator Research Program"— Presentation transcript:

1 US LHC Accelerator Research Program
bnl - fnal- lbnl - slac Preliminary simulations of e-cloud feedback in the SPS with Warp-POSINST J.-L. Vay, M.A. Furman LBNL Presented by M. Venturini (LBNL) E-cloud mitigation mini-workshop CERN - November 20-21, 2008 E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

2 Warp - 3D accelerator/PIC code
Geometry: 3D, (x,y), (x,z) or (r,z) Field solvers: electrostatic - FFT, capacity matrix, multigrid, AMR electromagnetic - Yee mesh, PML bc, AMR Particle movers: Boris, “drift-kinetic”, new leapfrog Boundaries: “cut-cell” --- no restriction to “Legos” (not in EM yet) Lattice: general; takes MAD input solenoids, dipoles, quads, sextupoles, … arbitrary fields, acceleration Bends: “warped” coordinates; no “reference orbit” Diagnostics: Extensive snapshots and histories Python and Fortran: “steerable,” input decks are programs Parallel: MPI Misc.: tracing, quasistatic modes, support for boosted frame E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

3 Warp: Quasi-Static Mode (“QSM”)
2-D slab of electrons 3-D beam s lattice s0 bend drift quad 2-D slab of electrons (macroparticles) is stepped backward (with small time steps) through the frozen beam field 2-D electron fields are stacked in a 3-D array, push 3-D proton beam (with large time steps) using maps - “WARP-QSM” - as in HEADTAIL (CERN) or Leap-Frog - “WARP-QSL” - as in QUICKPIC (UCLA/USC). On parallel computers: (16 procs) proc N/ N/ N N Station n n n+N/ n-N/ n+N n+N-1 E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

4 feedback simulations - JL Vay, M Furman
Study feedback of EC induced single-bunch instability in smooth SPS lattice SPS at injection (Eb=26 GeV) =27.729 Np=1.11011 continuous focusing x,y= 33.85, 71.87 x,y= 26.12, z= Nstn ecloud stations/turn=100 Fresh e-cloud density as pre-computed by POSINST Initial e-cloud distribution in a bend (POSINST) E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

5 feedback simulations - JL Vay, M Furman
Feedback model 1 Highly idealized model of feedback system. Record slice centroid y0(t) from every beam passage *apply low-pass FFT filter (sharp cutoff at 800MHz): y0(t)=>ŷ0(t) scale transverse position y => y-gŷ0 (g=0.1 used in all runs) *optional stage E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

6 feedback simulations - JL Vay, M Furman
Preliminary simul. study of SPS EC feedback Model 1 - beam distribution after 300 turns Feedback OFF Feedback ON - cutoff 0.8GHz tail head tail head Y (cm) centroid Y (cm) head tail head tail Y-centroid (cm) Y-centroid (cm) unfiltered Filtered (FFT-cutoff 0.8GHz) Time (ns) Time (ns) Power (a.u.) Power (a.u.) unfiltered Filtered (FFT-cutoff 0.8GHz) Frequency (GHz) Frequency (GHz) E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

7 Controlling centroid motion reduces emittance growth
Evolution of emittance No feedback FB applied every turn (disclaimer: all simulations done with same resolutions but no guarantee of numerical convergence) E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

8 Feedback model 2 - prediction from two turns
record centroid offset y0(t) and y1(t) from two consecutive beam passages predict y2(t) from y1(t) and y0(t) using linear maps, ignoring longitudinal motion and effects from electrons *scale according to line charge density : y2(t) => y2(t) w *apply low-pass FFT filter (sharp cutoff at 800MHz): y2(t)=>ŷ2(t) one turn later, scale transverse position y => y-gŷ (g=0.1) *optional stage E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

9 feedback simulations - JL Vay, M Furman
Feedback is effective at lower e-cloud density Model 2 - ne~1.5x1012 m-3 No feedback filter off, w off filter on, w off X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical Emittance growth <1% Emittance growth <1% Emittance growth ~7.5% 300 turns average y-centroid average y-centroid average y-centroid average y-centroid 0.8GHz spectrum vs time spectrum vs time spectrum vs time E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

10 feedback simulations - JL Vay, M Furman
800 MHz bandwith too narrow at larger e-density Model 2 - ne~6x1012 m-3 No feedback filter off, w off filter on, w off X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical Emittance growth ~9% Emittance growth ~0.6% Emittance growth ~26% average y-centroid average y-centroid average y-centroid E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

11 Feedback model 3 – prediction from three turns
record centroid offset y0(t), y1(t) and y2(t) from three consecutive beam passages predict y3(t) from y0-2(t) using linear maps, ignoring longitudinal motion and effects from electrons *scale according to line charge density : y2(t) => y2(t) w *apply low-pass FFT filter (sharp cutoff at 800MHz): y2(t)=>ŷ2(t) one turn later, scale transverse position y => y-gŷ (g=0.1) *optional stage E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

12 Preliminary simul. study of SPS EC feedback Model 3 - ne~6x1012 m-3
No feedback filter off, w off filter on, w off filter off, w on filter on, w on X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical Emittance growth ~0.26% Emittance growth ~9% Emittance growth ~4.2% Emittance growth ~2.1% Emittance growth ~15% average y-centroid average y-centroid average y-centroid average y-centroid average y-centroid 300 turns E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

13 Tentative Conclusions
Work on determining the theoretical feasibility of a feedback system for e-cloud induced instability has just started. A (demanding) 800 MHz bandwidth system has been shown to provide the desired damping (at least for not too-large e-density) for the SPS case study considered damping the coherent vertical motion has beneficial impact on emittance growth More extensive study will be necessary to determine bandwidth requirement and should include more realistic modeling of feedback systems (filter, time delays, noise …) more complete modeling of beam dynamics (chromaticities …_ Developing a simplified model of beam-e-cloud interaction may be helpful for the process of optimizing feedback design (John Byrd) is modeling of e-cloud using effective wake-potential a viable option? E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

14 to follow is a short summary of recent work done by Joel Thompson with Wolfgang Hofle, Giovanni Rumolo, and John Byrd

15 EC Feedback with HEADTAIL
Goal: add simple active feedback module to HEADTAIL code to explore gain and bandwidth required to damp SPS ECI. No FB Perfect slice FB

16 FB Simulation Results FB on average vertical position ineffective (i.e. dipole FB) FB Bandwidth limitation implemented as a simple windowing function FB effective for bandwidths as low as 300 MHz Bandwidth below 500 MHz appears to require very large gain Proper kick phase determined from combination of position measurement from two consecutive turns. Summary: good initial results. Significantly more effort required.

17 feedback simulations - JL Vay, M Furman
BACKUPS E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

18 Preliminary simul. study of SPS EC feedback Model 2 - ne~1.5x1012 m-3
No feedback filter off, w off filter on, w off filter off, w on filter on, w on X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical Emittance growth <1% Emittance growth ~7.5% Emittance growth <1% Emittance growth <1% Emittance growth <1% 300 turns average y-centroid average y-centroid average y-centroid average y-centroid average y-centroid 300 turns E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

19 Preliminary simul. study of SPS EC feedback Model 2 - ne~6x1012 m-3
No feedback filter off, w off filter on, w off filter off, w on filter on, w on X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical X-horizontal Y-vertical Emittance growth ~9% Emittance growth ~0.6% Emittance growth ~1% Emittance growth ~26% Emittance growth ~92% average y-centroid average y-centroid average y-centroid average y-centroid average y-centroid 300 turns E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

20 POSINST provides advanced SEY model.
Monte-Carlo generation of electrons with energy and angular dependence. Three components of emitted electrons: backscattered: rediffused: true secondaries: I0 Ie Ir Its true sec. Phenomenological model: based as much as possible on data for  and d/dE not unique (use simplest assumptions whenever data is not available) many adjustable parameters, fixed by fitting  and d/dE to data back-scattered elastic re-diffused E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

21 WARP-POSINST unique features
merge of WARP & POSINST Key: operational; partially implemented (4/28/06) new e-/gas modules 2 1 + Adaptive Mesh Refinement Z R concentrates resolution only where it is needed 3 Speed-up x10-104 beam quad e- motion in a quad + Novel e- mover Allows large time step greater than cyclotron period with smooth transition from magnetized to non-magnetized regions 4 Speed-up x10-100 E-cloud mitigation, CERN, Nov. 2008 feedback simulations - JL Vay, M Furman

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