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Penco, G.

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MOOB04 Impact on a Seeded Harmonic Generation FEL of an Initial Energy Chirp and Curvature in the Electron Bunch Energy Distribution 27
 
  • A.A. Lutman, R. Vescovo
    DEEI, Trieste
  • P. Craievich, G. Penco
    ELETTRA, Basovizza
  • J. Wu
    SLAC, Menlo Park, California
 
 

In a harmonic generation free electron laser (HG FEL), the electron beam entering the undulator can have an initial energy curvature besides an initial energy chirp. Solving the Vlasov-Maxwell equations within the 1D model, we derive an expression for the Green function for the seeded HG FEL process for the case of the electron beam having both an energy chirp and an energy curvature. We give an asymptotic closed form which is a good approximation in the exponential growth regime, and a series expression that allows the evaluation of the field envelope along the undulator in both lethargy and exponential growth regime. The latter is useful to study the HG FEL behavior in the short modulator, like that of the FERMI@Elettra project. The FEL radiation properties such as central frequency shift and frequency chirp are studied considering Gaussian laser seeds of different temporal duration in respect to the Green functions temporal duration. The energy chirp and curvature of the electron bunch result in a time dependent bunching factor for the FEL start-up process in the radiator of the HG FEL like the FERMI@Elettra. The coherence properties of the FEL are examined.

 

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Slides

 
WEPC55 FEL Commissioning of the First Stage of FERMI@Elettra 635
 
  • G. De Ninno
    University of Nova Gorica, Nova Gorica
  • E. Allaria, M. Cornacchia, G. De Ninno, S. Di Mitri, B. Diviacco, G. Penco, C. Spezzani, M. Trovò
    ELETTRA, Basovizza
 
 

The commissioning of the first stage of FERMI@Elettra will start during the summer 2009. During the first year of operation, efforts will concentrate on the optimization of the gun performance, as well as of the electron-beam acceleration and transport through the LINAC. By fall 2010, it is our aim to generate out of the LINAC an electron beam as similar as possible to the one needed for obtaining the nominal (i.e., user-required) FEL performance [see, e.g., S. Di Mitri et al., this Conference]. Such a beam will be then injected into the undulator chain and used to get the first FEL light. In this paper, we present our strategy for the commissioning of the FEL process, both in SASE and seeded configurations. On the basis of start-to-end simulations, we also discuss the expected FEL performance for day-one operation.