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Additional resources for Beam Techniques (Control, Manipulation)
Beam Instrumentation”, CERN-PE-ED 001-92 (1992), rev. (1994). H. C. 1, CERN/SL/90-13, 1991. T. Lohse and P. Emma, “Linear Fitting of BPM Orbits and Lattice Parameters”, SLAC Single Pass Collider Memo CN-371 (1989). Y. Cai, M. Donald, J. Irwin, Y. Yan, “LEGO: A Modular Accelerator Design Code”, Proc. of IEEE PAC97, Vancouver, and SLAC-PUB-7642 (1997). The RESOLVE program was written by M. Lee. 27 27. J. Safranek, “Experimental determination of storage ring optics using orbit response measurements”, Nucl.
Tune Measurements in the SPS as Multicycling machine”, Proc. of EPAC96, Sitges (1996). D. , “Design and functionality of the LEP Q-meter”, Proc. of EPAC90, Nice (1990). J. Borer and R. Jung, “Diagnostics”, CERN Accelerator School on Antiprotons for Colliding Beam Facilities, CERN 84-15, p. 385 (1984) R. Bartolini, M. Giovannozzi, W. Scandale, A. Verdier, C. Pellegrini, P. Tran, E. Todesco, J. Corbett, M. Cornacchia, “Measurements of the Tune Variations Induced by Non-Linearities in Lepton Machines”, Proc.
5: Comparison of measured data (solid curve) and amplitude fit (dashed curve). Plotted are the horizontal and vertical beam positions as measured as a function of distance along the transport line. See also ref. 4 . errors in the quadrupoles, random errors in the BPM gains, or wakefields, which are not included in the model. Nonetheless, the dynamics are predictable by incorporating the fitted errors into the accelerator model. 6: Comparison of measured data and fit to betatron amplitude only (a) or fit to both betatron amplitude and energy in the different linac sections (b).