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Beam-Beam Simulations Ji Qiang US LARP CM12 Collaboration Meeting Napa Valley, April 8-10, 2009 Lawrence Berkeley National Laboratory
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Outline Strong-strong beam-beam simulation for crab cavity compensation at LHC Strong-strong beam-beam simulation for conducting wire compensation at LHC
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Luminosity Loss from Crossing Angle Collision
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90 degree Crab Cavity Compensation Scheme
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BeamBeam3D: Parallel Strong-Strong / Strong-Weak Simulation Beam-Beam forces – integrated, shifted Green function method with FFT – O(N log(N)) computational cost Multiple-slice model for finite bunch length effects Parallel particle-based decomposition to achieve perfect load balance Lorentz boost to handle crossing angle collisions Arbitrary closed-orbit separation (static or time-dep) Multiple bunches, multiple collision points Linear transfer matrix + one turn chromaticity+thin lens sextupole kicks Conducting wire, crab cavity, and electron lens compensation
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x y Particle Domain -R2RR 0 A Schematic Plot of the Geometry of Two Colliding Beams Field Domain Head-on collision Long-range collision Crossing angle collision
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Green Function Solution of Poisson’s Equation ; r = (x, y) Direct summation of the convolution scales as N 4 !!!! N – grid number in each dimension
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Green Function Solution of Poisson’s Equation (cont’d) Hockney’s Algorithm:- scales as (2N) 2 log(2N) - Ref: Hockney and Easwood, Computer Simulation using Particles, McGraw-Hill Book Company, New York, 1985. Shifted Green function Algorithm:
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Comparison between Numerical Solution and Analytical Solution (Shifted Green Function) ExEx radius inside the particle domain
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Green Function Solution of Poisson’s Equation (Integrated Green Function) Integrated Green function Algorithm for large aspect ratio: x (sigma) EyEy
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IP Lab frame Moving frame: c cos( ) 2 Head-on Beam-Beam Collision with Crossing Angle
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Transform from the Lab Frame to the Boosted Moving Frame Refs: Hirata, Leunissen, et. al.
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Thin Lens Approximation for Crab Cavity Deflection
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B.Erdelyi and T.Sen, “Compensation of beam-beam effects in the Tevatron with wires,” (FNAL-TM-2268, 2004). Model of Conducting Wire Compensation (x p0,y p0 ) test particle
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Beam energy (TeV) 7 Protons per bunch 10.5e10 */ crab (m) 0.5/4000 Rms spot size (mm) 0.01592 Betatron tunes (0.31,0.32) Rms bunch length (m) 0.077 Synchrotron tune 0.0019 Momentum spread 0.111e-3 Crab cavity RF frequency 400.8 MHz LHC Physical Parameters for Testing Crab Cavity
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IP5 CAB 21 A Schematic Plot of LHC Collision at 1 IP and Crab Cavities IP
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One Turn Transfer Map with Beam-Beam and Crab Cavity M = Ma M1 Mb M1 -1 M M2 -1 Mc M2 Ma: transfer map from head-on crossing angle beam-beam collision Mb,c: transfer maps from crab cavity deflection M1-2: transfer maps between crab cavity and collision point M: one turn transfer map of machine
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Luminoisty Evolution with 0.15 mrad Half Crossing Angle with/without Crab Cavity turn
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Luminosity vs. Beta* for LHC Crab Cavity Compensation with crab cavity no crab cavity
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Correlated Random Error Time-dependent Error Effects of Phase Jitter
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Emittance Growth/Per Hour vs. Random Offset Amplitude (beta*=0.25, preliminary results, voltage mismatch)
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Emittance Growth/Per Hour vs. Time Modulated Amplitude (beta* = 0.25, preliminary results, voltage mismatch)
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Emittance Growth with 0.85 um random offset without/with Correction
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IP1 IP5 Strong-Strong Beam-Beam Simulation LHC Wire Compensation (2 Head-On + 64 Long Range)
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peak luminosity evolution with conduting wire compensation and reduced separation
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Strong-Strong Beam-Beam Simulation LHC Wire Compensation: effect of wire current fluctuation
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