Computing for accelerator physics Ilya Agapov, 7/12/09, DESY ...

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Energy deposition, collimation, halo and backgrounds at ILC ILC collimation system (top left), electron and photon halo (top right) power losses in the extraction line (bottom left), energy deposition in a final focus quadrupole (bottom right) 30
Start to end simulations Several codes staged to simulate the whole accelerator, typically from injector to the experimental station IMPACTT (Photoinjector), ELEGANT (Accelerator), Genesis (FEL process) for LCLS (Y Ding et al.) ASTRA + ELEGANT for PSI injector test facility (Y. KIM et al.) ASTRA + ELEGANT + + CSRTRACK + GENESIS for DESY XFEL MERLINbased for ILC (D. Krucker et al.) PLACET + BDSIM for CLIC (codes run in parallel, PLACET compute the wakefields and BDSIM tracks the secondaries and computes energy deposition)
Page 1 and 2: Computing for accelerator physics I
Page 3 and 4: Areas where computing plays a role
Page 5 and 6: Linear accelerators Injectorts for
Page 8 and 9: Plasmawakefield acceleration Use
Page 10 and 11: EM field calculations LHC main quad
Page 12 and 13: CST particle studio Collimator wake
Page 14 and 15: Wakefield code ECHO (TU Darmstadt /
Page 16 and 17: Beam optics Accelerator dimensions
Page 18 and 19: Linear optics A typical parametriza
Page 20: Steering (PLACET code, D.Schulte, A
Page 26 and 27: MADX Widely used beam optics cod
Page 28 and 29: Energy deposition and machinedete
Page 32 and 33: Control Systems and online optics
Page 34 and 35: LHC Online model Provide virtual
Page 36 and 37: User interface for interactive expe
Page 38 and 39: Aperture measurements (arcs) Free
Page 40 and 41: General data management issues Dat

Computing for accelerator physics Ilya Agapov, 7/12/09, DESY ...

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