The tandem FEL dynamic behavior

A tandem FEL consists of two conventional FEL oscillators separated by a drift section. The same e-beam drives both oscillators, and since the first oscillator, where conventional evolution occurs, pilots the behavior of the second, an interesting dynamic behavior arises. We discuss the dynamic aspects of the problem from low signal to saturation, analyze the efficiency of the device, and present preliminary design considerations. >

[1]  Torre,et al.  Dynamical behavior of a free-electron laser operating with a prebunched electron beam. , 1994, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[2]  G. Dattoli,et al.  Saturation dynamics in FEL and optical-klystron FEL devices , 1994 .

[3]  G. Dattoli,et al.  Design elements of a high-power VUV free electron laser , 1993 .

[4]  Torre,et al.  Saturation and cavity-loss optimization in free-electron lasers. , 1993, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[5]  D. C. Quimby,et al.  CW 100 kW radio frequency-free-electron laser design at 10 mu m , 1991 .

[6]  Yu,et al.  Generation of intense uv radiation by subharmonically seeded single-pass free-electron lasers. , 1991, Physical review. A, Atomic, molecular, and optical physics.

[7]  R. Bonifacio,et al.  Generation of XUV light by resonant frequency tripling in a two-wiggler FEL amplifier☆ , 1990 .

[8]  J. Madey,et al.  Initial Results From The Free-electron-laser Master Oscillator/Power Amplifier Experiment , 1989, Proceedings of the Eleventh International Free Electron Laser Conference.

[9]  Bamford,et al.  Measurement of the coherent harmonic emission from a free-electron laser oscillator. , 1989, Physical review letters.

[10]  J. Madey,et al.  Design concept for a common rf accelerator driven free electron laser master oscillator/power amplifier , 1988 .

[11]  C. Bazin,et al.  Optical properties of multilayer mirrors exposed to synchrotron radiation , 1988 .