Titlebook: Synchrotron Light Sources and Free-Electron Lasers; Accelerator Physics, Eberhard J. Jaeschke,Shaukat Khan,Jerome B. Hastin Reference work

Systemic

High-Gain Free-Electron Laser Theory, Introductionfor FEL gain. For 1D theory, we start from the resonance condition and energy exchange between electron and radiation field. Their dynamics are then derived as the coupled Maxwell-Vlasov equations using a fluid model. In solving these coupled equations, we introduce some important FEL parameters and

pacific

Self-Seeded Free-Electron Lasersency range where external seeding is not available. Schematically, it is composed of three parts: a Self-Amplified Spontaneous Emission (SASE) FEL working in the linear regime, a monochromator, and an FEL amplifier. Active filtering is achieved by letting the FEL pulse produced in the SASE FEL throu

ARY

Headstrong

Brilliant Light Sources Driven by Laser-Plasma Acceleratorse sciences to fundamental physics, as they enable new insights into processes on atomic length and time scales. Laser-plasma accelerators bear the promise to drive future compact free-electron lasers. A high-energy laser pulse excites a density perturbation in a plasma, generating large electric fie

高歌

Finasteride

FLASH: The First Superconducting X-Ray Free-Electron LaserThis chapter reports on the concept of the superconducting accelerator, the generation and formation of the electron bunches needed to drive the single-pass FEL process, and the performance of the FEL. Operation experience and upgrade programs like FLASH II are also described.

脖子

The Linac Coherent Light Source: Concept Development and Design Considerationscted the interest of accelerator physicists in the synchrotron light source community. Interest among x-ray researchers grew slowly until about 1996, when scientists at DESY produced a concept for a large x-ray laser research facility (now the European XFEL). The US Department of Energy (DOE) conduc

忍耐

The SACLA X-Ray Free-Electron Laser Based on Normal-Conducting C-Band Technologyfrom 1996 ∼ 2000, guided by the author at KEK (Group .; Shintake et al. ., .), followed by SCSS project (Shintake et al. ., .; Group .) at RIKEN/SPring-8 (2001 ∼ 2005), where we demonstrated high-gradient operation of a C-band accelerator. Based on the developed C-band technology, 400-m-long 8-GeV C

Patrimony

Inelasticity

Integrated Multimagnet Systemssions as a consequence. There are several reasons for this: .This chapter describes the technology of integrating several magnets in a common steel block. Several new system properties are presented in the chapter: .This chapter first describes the MAX IV integrated multi-magnet system in quite some