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Theory of high gain free-electron lasers operating with segmented undulators
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10.1063/1.2171810
/content/aip/journal/jap/99/4/10.1063/1.2171810
http://aip.metastore.ingenta.com/content/aip/journal/jap/99/4/10.1063/1.2171810
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Power of the fundamental harmonic (units in megawatts) vs , total relative energy spread vs z, and square modulus of the first five bunching coefficients vs . Simulation parameters: , , , , and operating wavelength .

Image of FIG. 2.
FIG. 2.

(a) Evolution of the FEL power in a segmented undulator configuration. The first section is provided by an undulator with the same characteristic as before, and the second section by an undulator with , . Furthermore , , and the operating wavelength in the second undulator is . (b) Evolution of the FEL evolution in a nonsegmented configuration. The simulation parameters are those of the second section of the previous case (a).

Image of FIG. 3.
FIG. 3.

Comparison between numerical and semianalytical results for the case of Fig. 2(a).

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/content/aip/journal/jap/99/4/10.1063/1.2171810
2006-02-23
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Theory of high gain free-electron lasers operating with segmented undulators
http://aip.metastore.ingenta.com/content/aip/journal/jap/99/4/10.1063/1.2171810
10.1063/1.2171810
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