LARP Accelerator Physics 19 June 2008 LARP+LAUC DOE Review, LBNL Wolfram Fischer/BNL BNL - FNAL- LBNL - SLAC US LHC Accelerator Research Program.

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Presentation transcript:

LARP Accelerator Physics 19 June 2008 LARP+LAUC DOE Review, LBNL Wolfram Fischer/BNL BNL - FNAL- LBNL - SLAC US LHC Accelerator Research Program

Accelerator Physics Tasks in FY Electron cloud studies – M. Furman (LBNL) 2.Beam-beam wire compensation – W. Fischer (BNL) 3.Beam-beam simulations – T. Sen (FNAL) 4.Electron lenses – V. Shiltsev (FNAL) 5.Crab cavities – R. Calaga (BNL) 6.New initiatives – T. Markiewicz (SLAC) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 2 Total AP effort: ~ 4-5 FTEs

Task: Electron cloud studies (M. Furman, LBNL) Goal: simulate electron cloud effects in the LHC and the LHC injectors in order to optimize the operation and design of these machines when limited by electron clouds. Activities in reporting period: Benchmark WARP vs. HEADTAIL (emittance evolution) Benchmark POSINST(2D) vs. WARP(2D) and (3D) (build-up) E-cloud build-up simulation of SPS strip detector measurement SPS feedback simulations (started) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 3

Task: Electron cloud studies (M. Furman, LBNL) Benchmark WARP vs. HEADTAIL-3 for incoherent emittance growth LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 4

Task: Electron cloud studies (M. Furman, LBNL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 5 Preliminary simulation study of SPS feedback

Tentative electron cloud task for FY2009 Consolidate new and existing electron cloud activities Emphasis on instability remedies in SPS SPS performance with LHC design beams marginal due to electron cloud induced instability Design of an instability feedback (J. Fox, SLAC) Simulations in support of feedback design (M. Furman, LBL) Test of grooved chambers (M. Pivi, SLAC) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 6

Tentative electron cloud task for FY2009 GROOVE TESTS IN THE SPS: A number of electron cloud mitigation test chambers are in preparation for installation in a new dedicated 4-magnet chicane in the SPS. At CERN/SLAC, we are manufacturing groove insertions to fit in one of the test chamber. The stringent requirements for a largest possible SPS chamber aperture call for a maximum 1mm height of the groove insertion. This requirement imposes tight tolerances on the sharpness of the groove tips and valley to reduce the secondary electron yield. We are investigating the manufacturing feasibility with different techniques: grounding (CERN), metal folding (SLAC), razor blades (SLAC). People: Venturini, Furman (LBNL), Pivi, Wang (SLAC) Arduini, Chapochnikova, Taborelli (CERN). LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 7 Metal Folding: Form multiple folds. [EMEGA Company, USA] Brazed-up Assembly: Use individual razor type foil blades

Task: Beam-beam wire compensation (W. Fischer, BNL) Goal: provide experimental data for long-range beam-beam effects as strong as in the LHC that can be used to benchmark beam-beam simulation codes No existing hadron machine has a long-range beam-beam effect as strong as LHC (~30 long-range interactions per IP) 2 wires designed, constructed and installed in RHIC to create strong long-range beam-beam effect Measurements done with Au and d beam so far (loss rate vs. distance, current, tune chromaticity) Proton measurements outstanding, task then finished LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 8

Task: Beam-beam wire compensation (W. Fischer, BNL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 9 Vertically movable wires in RHIC tunnel. Max integrated strength 125 Am (80 Am needed for compensators in LHC, 2x/IP).

Task: Beam-beam wire compensation (W. Fischer, BNL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 10 Beam loss rate vs. wire position and current with d beam in Jan Had also planned to make scans with p and including head-on effect. But only short (3.5 wks) RHIC physics run with protons – no experimental time. Plan to perform proton scans in FY2009.

Task: Beam-beam simulations (T. Sen, FNAL) Goal: benchmark beam-beam simulations codes with experimental data, currently primarily from RHIC, and evaluate the LHC beam-beam performance with long-range and head-on beam-beam compensation as well as for crab cavities. FNAL – H.J. Kim and T. Sen (BBSIM) Weak-strong, for SPS and RHIC wire experiments SLAC – A. Kabel (PlibB) Weak-strong, for RHIC wire experiments and e-lens LBL – J. Qiang (Beambeam3D) Strong-strong, for RHIC and LHC emittance growth LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 11

Task: Beam-beam simulations (T. Sen, FNAL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 12 Simulated and measured beam loss rate as function of wire distance (RHIC d scan, 1/2008) Courtesy H.J. Kim, T. Sen, FNAL Onset of increased beam loss rate could be reproduced within 1  for a number of the RHIC scans made. (independently also by U. Dorda, CERN, with Code BBTrack)

Task: Beam-beam simulations (T. Sen, FNAL) Emittance growth from diffusion coefficients Emittance growth may be driven by diffusive processes in the core, dynamics in the tails, which determine lifetime, may not be diffusive Calculate diffusion coefficients from BBSIM and use as input in independent diffusion solver Evolve density and moments to find emittance growth and lifetime over relevant time periods (hours) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 13 RHIC d beam (store 9572) Courtesy H.J. Kim, T. Sen

Task: Beam-beam simulations (T. Sen, FNAL) Physics additions to simulation programs (recent or future): BBSIM (FNAL) Coupling (Edward-Teng) Resistive wall wakefield Symplectic synchro-beam map PlibB (SLAC) MAD-X lattice input (i.e. full LHC files) Intrabeam scattering Electron lens BeamBeam3D Crab cavities – impact of phase noise LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 14

Task: Beam-beam simulations (T. Sen, FNAL) Planned work for FY2009: Evaluate wire compensation in LHC and benefit to luminosity Simulate wire compensation in RHIC and compare with measurements in FY2009 Improve the diffusion model: add other sources of diffusion in tracking, use diffusion equation in 3D action space. Extend the comparison to other stores. Evaluate the impact of crab cavities in the LHC with weak-strong and strong-strong simulations. Set tolerances on noise parameters. Evaluate electron lenses in the LHC LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 15

Task: Electron lenses (V. Shiltsev, FNAL) Goal: evaluate the LHC luminosity improvement with electron lenses for head-on beam-beam compensation, and other possible applications of electron lenses Reducing tune footprints is not sufficient Work includes Experiments in the Tevatron with a Gaussian profile lens Numerical simulations Theoretical analysis Electron lenses could be included in the Phase II LHC IR upgrade. LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 16

Task: Electron lenses (V. Shiltsev, FNAL) Need Gaussian gun for head-on compensation Current TEL lenses have flat profile with soft edges Built Gaussian profile gun for test (awaiting installation) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 17 Courtesy V. Kamerdzhiev Planned Tevatron experiments: Effect on of e-lens on tune spread Determine tolerable noise levels (position, current)

Task: Electron lenses (V. Shiltsev, FNAL) Numerical simulations, approach Show that beam-beam effect becomes unacceptable above certain beam-beam parameter  Turn on electron lenses to see improvement Not straight forward to determine acceptable beam-beam parameter  Figures of merit investigated: Short-term measures (tune footprint, tune and action diffusion, chaotic boarders) are all inconclusive when taken alone Dynamic aperture not a good measure for beam-beam problems Emittance growth probably too noisy signal in simulation Beam lifetime most promising but need a good model and sufficient CPU time LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 18

Task: Electron lenses (V. Shiltsev, FNAL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 19 LHC simulation with LIFETRACK different phase advances between IP and e-lens (  =  with linear lattice and ideal e-lens is optimum) Lifetime simulations need benchmarking with existing machines (Tevatron, RHIC) Courtesy A. Valishev

Task: Electron lenses (V. Shiltsev, FNAL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 20 Related work: e-lens simulation study at RHIC – Y. Luo No BB BB Half comp.Full comp.

Tentative beam-beam task for FY2009 RHIC wire experiments are winding down Electron lens effort is ramping up Plan to consolidate all 3 existing beam-beam tasks into one Emphasis on electron lenses Simulation support also shifting from RHIC wire experiments to electron lenses and crab cavities LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 21

Task: Crab cavities (R. Calaga, BNL) Goal: design, construction and installation of a crab cavity in the LHC, and the evaluation of its potential for luminosity upgrades. Crab cavities necessary for early separation scheme (D0) 800 MHz cavity under design (  c < 0.6 mrad), could be built by AES/BNL with SBIR grant (no SBIR grant this year) – workshop CC’08 Study items Emittance growth from rf noise Collimation and machine protection Aim for late 2009 workshop at CERN after which CERN commits to install a single prototype at IP4 (rf section) in LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 22

Task: Crab cavities (R. Calaga, BNL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 23 In upgrade version with D0 crab cavities increase luminosity, especially with small  * (unlike KEKB no increase in beam-beam parameter targeted)

Task: Crab cavities (R. Calaga, BNL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 24 Phased test and upgrade plan

Task: Crab cavities (R. Calaga, BNL) LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 25 Cavity design status

Tentative Accelerator Physics Tasks in FY Electron cloud studies – M. Pivi (SLAC) SPS instability feedback design Simulations Grooved chambers in SPS 2.Beam-beam – ? Electron lenses Simulations Wire compensation 3.Crab cavities – R. Calaga (BNL) Cavity and cryostat design Couplers and tuners Simulations 4.CERN PS2 studies – U. Wienands (SLAC) With participation of BNL, LBL, FNAL, SLAC LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 26

New Task: CERN PS2 studies (U. Wienands, SLAC) Goal: Support the design of the PS2 (replacement machine for the PS). Design of PS2 approved by CERN Council in June LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 27

New Task: CERN PS2 studies (U. Wienands, SLAC) Scope and budget are under discussion Synergies with the FNAL MI upgrade Interest from all 4 LARP labs Involvement of one Toohig Fellow (R. DeMaria) Critical issue is loss control (1W/m – FODO lattice vs. imaginary  t ) 3 possible packages 1.Tracking, nonlinearities, space charge, halos, H - injection 2.Intensity effects, instabilities 3.RF system LARP could make a visible contribution. LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 28

Summary – LARP Accelerator Physics Two themes: 1.Consolidation of existing tasks: Electron cloud task new focus on SPS instability, supporting instability feedback design, chamber R&D and simulations Beam-beam task all beam-beam work in one task (so far 3), new focus on e-lenses 2.New or significantly larger tasks: Crab cavities, supporting design of cavity CERN PS2, design studies, scope and budget under discussion LARP+LAUC DOE Review – June 2008LARP Accelerator Physics - W. FischerSlide n° 29