Large Scale Parallel Wake Field Computations with PBCI

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1 Large Scale Parallel Wake Field Computations with PBCI E. Gjonaj, X. Dong, R. Hampel, M. Kärkkäinen, T. Lau, W.F.O. Müller and T. Weiland ICAP `06 Chamonix, 2-6 October 2006 Technische Universität Darmstadt, Fachbereich Elektrotechnik und Informationstechnik Schloßgartenstr. 8, Darmstadt, Germany - URL:

2 Outline Introduction Numerical Method Parallelization Strategy Modal Termination of Beam Pipes PBCI Simulation Examples Conclusions 1

3 Introduction Motivation for PBCI: 1. A new generation of LINACs with ultra-short electron bunches a. bunch size for ILC: 300 μm 2 b. bunch size for LCLS: 20 μm 2. Geometry of tapers, collimators far from rotational a. 8 rectangular collimators at ILC-ESA in the design process b. 30 rectangular-to to-round transitions in the undulator of LCLS 3. Many (semi-) analytical approximations become invalid a. based on rotationally symmetric geometry b. low frequency assumptions (Yokoya, Stupakov) c. detailed physics needed for high frequency wakes (Bane)

4 Introduction beam view side view 15.05mm 38.1mm mm 38.05mm 17.65mm mm Courtesy: N. Watson, Birmingham 1 m 38.05mm ILC-ESA collimator #3 ILC-ESA collimator #8 bunch length 300μm collimator length ~1.2m catch-up distance ~2.4m

5 Introduction vacuum vessel tube shielding PITZ diagnostics double cross gap outgoing pipe step bunch length bunch width 2.5mm 2.5mm bunch length taper length 1cm 50cm structure length 325mm Tapered III vacuum slots elliptic pipe 4 Courtesy: R. Wanzenberg, DESY

6 Introduction There is an actual demand for: 1. Wake field simulations in arbitrary 3D-geometry 3D-codes 2. Accurate numerical solutions for high frequency fields (quasi-) dispersionless codes 3. Utilizing large computational resources for ultra-short bunches parallelized codes 4. Specialized algorithms for long accelerator structures moving window codes 5

7 An (incomplete) survey of available codes Introduction Dimensions Nondispersive Parallelized Moving window 1982 BCI / TBCI 2.5D No No Yes Time NOVO ABCI MAFIA GdfidL ECHO PBCI 2.5D 2.5D 2.5/3D 3D 2.5/3D 3D Yes No No No Yes Yes No No No Yes No Yes No Yes No No Yes Yes 6

8 Outline Introduction Numerical Method Parallelization Strategy Modal Termination of Beam Pipes PBCI Simulation Examples Conclusions 7

9 Numerical Method The FIT discretization 8 A A V V E ds = μ H da t A H ds = ε E + J da t A μ H da= 0 εe da= Topology of FIT: V ρ dv FIT Ce = d dt M h μ d Ch = M ε e + j dt SM e q ε = SMμ h = C T = C semidiscrete energy conservation SC = SC = 0 semidiscrete charge conservation 0

10 Numerical Method Using the conventional leapfrog time integration n+ 1/2 1 T n 1/2 n e Δt e 1 M 1 ε C t ε n+ 1 = Δ T n M j Δt μ Δt h M C 1 MμCMε C h Behavior of numerical phase velocity vs. propagation angle cδt 1 σ : = Δz Stable but large dispersion z cδt σ : = = 1 Δz No dispersion but unstable z

11 Numerical Method Idea: Reduce the integration of 3D equations to a sequence of 1D / 2D integrations along the coordinate axes Longitudinal-Transversal (LT) splitting: 10 H H t l 1 T 0 Mε C t = 1 Mμ Ct 0 does not affect longitudinal waves 1 T 0 M ε Cl = 1 Mμ Cl 0 integrable in 1D without numerical dispersion n+ 1 n n Δt Δt t t t Δ 2 lδt 2 3 e = e e H H = e e e e H H + O( Δt ) modified time evolution h h h Second order Strang splitting

12 Numerical Method Idea: Reduce the integration of 3D equations to a sequence of 1D / 2D integrations along the coordinate axes Replace each evolution operator with Verlet-leapfrog propagators: 11 G 2 3 Δt 1 T 1 1 T Δt 1 T 1 1 T 1 Mε Clt ; MμClt ; ΔtMε Clt ; Mε Clt ; MμClt ; Mε Clt ; 2 4 Δ = 2 ( t) lt ; 2 1 Δ t 1 1 T ΔtMμClt ; 1 MμClt ; Mε Clt ; Time discrete update: n+ 1 e Δt Δt e = Gt igl( Δt) igt i h 2 2 h T. Lau, E. Gjonaj and T. Weiland, Time Integration Methods for Particle Beam Simulations with the Finite Integration Theory, FREQUENZ, Vol. 59 (2005), pp. 210 n cδt stable for: σ : = = 1 Δz

13 Implementing the LT splitting scheme n+ 1 e Δt Δt e = Gt igl( Δt) igt i h 2 2 h Numerical Method n 12 Numerical phase velocity and amplification vs. propagation angle cδt σ : = = 1 Δz No longitudinal dispersion z z Neutrally stable

14 Outline Introduction Numerical Method Parallelization Strategy Modal Termination of Beam Pipes PBCI Simulation Examples Conclusions 13

15 Parallelization Strategy A balanced domain partitioning approach total computational domain 14 W W N left right left = N N =, Nright = 2 2 N N left right intermediate subdomains processor #1 active subdomains binary tree leafs processor #2 processor #3 Equal loads assigned to each node: W = α i w Node Node i Grid Points

16 Parallelization Strategy Example: Tapered transition for PETRA III moving grid window Domain partitioning pattern for 7 processors 15 Total Min Max Dev. Grid points < 1.0% Number of Grid Points Distribution of grid points Processor Number

17 Parallelization Strategy 16 Speedup Parallel performance tests 10e5 Grid points 10e6 Grid points 50e6 Grid points 10e7 Grid points 20e7 Grid points Ideal Number of Processors TEMF Cluster: 20 INTEL 3.4GHz, 8GB RAM, 1Gbit/s Ethernet Network

18 Parallelization Strategy 1,2 Parallel performance tests 1 17 Efficiency 0,8 0,6 0,4 0,2 10e5 Grid points 10e6 Grid points 50e6 Grid points 10e7 Grid points 20e7 Grid points Ideal Number of processors TEMF Cluster: 20 INTEL 3.4GHz, 8GB RAM, 1Gbit/s Ethernet Network

19 Outline Introduction Numerical Method Parallelization Strategy Modal Termination of Beam Pipes PBCI Simulation Examples Conclusions 18

20 Modal Termination of Pipes y Indirect integration schemes C 2 C0 z = 0 C1 z 19 direct indirect 1 z+ s Wz() s = dzez(, z t ) Q = c 1 z+ s 1 TM s = dz Ez(, z t ) dy Gy (0, t ) Q = = c Q c C Indirect integration of potential for 2D-structures (Weiland 1983, Napoly 1993) 2. Generalization for 3D-structures (A. Henke and W. Bruns, EPAC 06, July 2006, Edinburgh, UK) TM G = e E + cb + e E cb + e E TM TM TM TM ( ) ( ) x x y y y x z z C irrotational

21 Modal Termination of Pipes y z = 0 Modal approach C0 C1 z 20 direct 1 z+ s Wz() s = dzez(, z t ) Q = c = n modal n 1 i( ω / c) s z(, ) ω n( ω) i ω c k ω e x y d C e ( / zn, ( )) 1 z+ s 1 n = dz Ez(, z t ) ez(, x y) Wn() s Q = c Q = + = = z s i n ikn ( ω) z c dz Ez( x, y, z, t ( z s)/ c) dz dω Cn( ω) ez( x, y) e e ω n C 0 W () n s n-th (TM) mode contribution n spectral coefficient of n-th (TM) mode

22 Modal Termination of Pipes 1. Time domain integration in the inhomogeneous sections: 0 1 z+ s dz Ez (, z t ) Q = c 21 n n 2. Modal analysis at z = 0: E ( x, y,0, t) E (0, t), e ( x, y) z z z n 3. Compute spectral coefficients (FFT): E (0, t) C ( ω) 4. Compute wake potential contribution per mode (IFFT): C n ( ω) ( ω/ zn, ( ω) ) i c k W n () s 5. Compute wake potential transition in the outgoing pipe: 1 z+ s 1 n dz Ez(, z t ) ez(, x y) Wn() s Q = = c Q 0 n z n

23 Modal Termination of Pipes Using FD reconstruction in long intermediate pipes diagnostics cross injector section bunch 22 1mm step full Time Domain E z / [kv /m] FD analysis reconstruction lowest eigenmodes bunch

24 Outline Introduction Numerical Method Parallelization Strategy Modal Termination of Beam Pipes PBCI Simulation Examples Conclusions 23

25 Simulation Examples TESLA 9-cell cavity bunch E z / [kv /m] bunch length 5mm bunch charge 1nC cavity length 1.5m no. of grid points ~80e6 no. of processors 24 simulation time 3hrs

26 Simulation Examples TESLA 9-cell cavity 5 Longitudinal wake potential 25 Wz / [V / pc] ,5 0 1,5 3 4,5 s / [cm] Bunch (a.u.) z = 20cm z = 40cm z = 60cm z = 80cm z = 100cm z = 120cm z = 140cm

27 PITZ diagnostics double cross Simulation Examples bunch E z / [kv /m] bunch size σ / Δz no. of grid points no. of processors simulation time 2.5mm 30 ~500e hrs Vacuum Vessel Gap Beam Tube Tube Shielding Step

28 PITZ diagnostics double cross 1 Simulation Examples (Ackermann, Hampel, Schnepp) Wake field impact of the single components 27 W z / [V / pc] cross with shielding tube full model no shielding tube gap (1 mm) step (no taper) s [mm]

29 Simulation Examples 28 ILC-ESA collimator #8 Wz / [V / pc] Convergence vs. grid step σ / Δz = 2.5 σ / Δz = 5 σ / Δz = 10 σ / Δz = 15 bunch size no. of grid points no. of processors simulation time s / σ 300μm ~450e hrs

30 Simulation Examples ILC-ESA collimator #8 Direct and transition wakes bunch mm mm 38.1 mm mm 2.75 mm mm 29 Wz / [V / pc] 30 Direct potential (z = 150mm) Transition potential Steady state potential s / σ

31 Conclusions 1. PBCI: A fully 3D- code for wake field simulations a. using the moving window approach b. dispersionless in the bunch propagation direction c. massively parallelized d. using modal approach for indirect integration e. using modal approach for pipe termination 2. Work still in progress for a. including resistive wall wakes b. developing an appropriate boundary conformal discretization c. considering periodic structures of finite length 30

32

33 General split-operator schemes d dt e 1 T 0 Mε C = 1 h Mμ C 0 h e Numerical Method (homogeneous) FIT equations 32 Denote: e y =, h Solution after one time step: d y dt 0 M C H = M C 0 1 T ε, 1 μ ( H H ) + 1 HΔ 1+ 2 Δt Hiy y e iy e iy = = = A second order Strang scheme: n t n n y n H= H1+ H2 exact time evolution operator approximate time evolution operator Δt Δt H H H2Δt 2 n = e e e i y + O( Δt )

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