Abstract

Linac driven free electron lasers (FELs) operating in the x-ray region require a high brightness electron beam in order to reach saturation within a reasonable distance in the undulator train or to enable sophisticated seeding schemes using external lasers. The beam dynamics optimization is usually a time consuming process in which many parameters of the accelerator and the compression system have to be controlled simultaneously. The requirements on the electron beam quality may also vary significantly with the particular application. For example, the beam dynamics optimization strategy for self-amplified spontaneous emission operation and seeded operation are rather different: seeded operation requires a more careful control of the beam uniformity over a relatively large portion of the longitudinal current distribution of the electron bunch and is therefore more challenging from an accelerator physics point of view. Multiobjective genetic algorithms are particularly well suited when the optimization of many parameters is targeting several objectives simultaneously, often with conflicting requirements. In this paper we propose a novel optimization strategy based on a combination of multiobjective optimization with a fast computation of the FEL performance. The application to the proposed UK's New Light Source is reported and the benefits of this method are highlighted.

Highlights

  • With the successful operation of the Linac Coherent Light Source (LCLS) in the USA [1], SACLA X-FEL in Japan [2], FERMI at ELETTRA in Italy [3], and FLASH in Germany [4], free electron lasers (FELs) operating in the x-ray region have been firmly established as powerful tools for enabling new scientific research

  • III we show the results of the application of multiobjective genetic algorithms (MOGA) to the optimization of the UK’s New Light Source (NLS) linac design [14]

  • spontaneous emission (SASE) and seeded FELs operating in the x-ray region usually require beams with kA peak current, with a normalized emittance lower than 1 m and energy spread in the order of 10À4

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Summary

Introduction

With the successful operation of the Linac Coherent Light Source (LCLS) in the USA [1], SACLA X-FEL in Japan [2], FERMI at ELETTRA in Italy [3], and FLASH in Germany [4], free electron lasers (FELs) operating in the x-ray region have been firmly established as powerful tools for enabling new scientific research. Most of the existing projects rely on a high brightness electron gun, followed by a linear accelerator to reach the operating energy, equipped with one or more magnetic compression stages to reach the required peak current. Maintaining high brightness during the acceleration and compression process is the main goal of beam dynamics optimization in the linac. The basic selfamplified spontaneous emission (SASE) mode of operation [5] demands a large peak current, small normalized emittance, and small energy spread. Each portion of the bunch with sufficient beam quality, and with a length equal to the FEL cooperation length, will radiate an independent SASE spike so that the time coherence of SASE pulses is limited. All slices with sufficient beam quality will lase independently and with different saturation lengths

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