Optimal Control of Gains in a Linear Accelerator: A Supervisory Method for Vector-Sum Control

In a linear accelerator, driven by radio frequency (RF) amplifier stations, one must precisely control the energy gain of the accelerating beam. The RF stations can be viewed as amplifiers placed sequentially to accelerate the beam. This brief presents two control schemes within which the RF stations act as actuators, and a centralized control unit controls the beam energy by acting either on the RF amplitudes or on the RF phases. The control algorithms are based on convex optimization problems with different objectives. The two approaches are successfully tested at the SwissFEL injector test facility using three full-scale RF stations. The two methods are compared from both performance and complexity points of view.

[1]  H. Schlarb,et al.  FAST FEEDBACK STRATEGIES FOR LONGITUDINAL BEAM STABILIZATION , 2016 .

[2]  Roy S. Smith,et al.  MPC based supervisory control design for a Free Electron Laser , 2015, 2015 54th IEEE Conference on Decision and Control (CDC).

[3]  Roy S. Smith,et al.  Beam-Based Power Distribution Over Multiple Klystrons in a Linear Accelerator , 2015 .

[4]  Herbert Werner,et al.  Distributed controller design for a free-electron laser , 2013, 2013 American Control Conference.

[5]  Maurizio Vretenar,et al.  Linear accelerators , 2013, 1303.6766.

[6]  Stephen P. Boyd,et al.  CVXGEN: a code generator for embedded convex optimization , 2011, Optimization and Engineering.

[7]  Christian Schmidt,et al.  RF system modeling and controller design for the European XFEL , 2011 .

[8]  Thomas P. Wangler,et al.  Principles RF Linear Accelerators: Wangler/Principles , 2008 .

[9]  L. Hendrickson Beam-based Feedback Testing and Simulations for the SLC Linac , 2000 .

[10]  D. A. G. Deacon,et al.  Free electron laser , 1978, Optics & Photonics.

[11]  John M. J. Madey,et al.  A Free Electron Laser , 1973 .

[12]  Zheqiao Geng,et al.  ARCHITECTURE DESIGN FOR THE SwissFEL LLRF SYSTEM , 2014 .

[13]  Zheqiao Geng,et al.  SwissFEL C-BAND LLRF PROTOTYPE SYSTEM , 2014 .

[14]  Amin Rezaeizadeh,et al.  Model-based klystron linearization in the SwissFEL test facility , 2014 .

[15]  G.Gaio,et al.  Evolution of the FERMI Beam Based Feedbacks , 2013 .

[16]  G. Penco,et al.  BEAM-BASED FEEDBACKS FOR THE FERMI @ Elettra FREE ELECTRON LASER , 2010 .

[17]  T. Schietinger,et al.  PHOTOCATHODE DRIVE LASER FOR SWISSFEL , 2010 .

[18]  C. Schmidt,et al.  INTRA-TRAIN LONGITUDINAL FEEDBACK FOR BEAM STABILIZATION AT FLASH , 2010 .

[19]  Marco Pedrozzi,et al.  CONCEPTUAL DESIGN OF THE C-BAND MODULE FOR THE SWISSFEL , 2010 .

[20]  Sincrotrone,et al.  BEAM-BASED FEEDBACKS FOR THE@Elettra FREE ELECTRON LASER , 2010 .

[21]  Injector Mission,et al.  250 MeV INJECTOR FACILITY FOR THE SwissFEL PROJECT M. Pedrozzi on behalf of the SwissFEL team Paul Scherrer Institute, 5232 Villigen PSI, Switzerland , 2009 .

[22]  Thomas Wangler,et al.  Principles of RF linear accelerators , 1998 .

[23]  T. Schilcher,et al.  Vector sum control of pulsed accelerating fields in Lorentz force detuned superconducting cavities , 1998 .