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Stability properties of free-electron laser in Raman regime with thermal electron beam
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10.1063/1.3106684
/content/aip/journal/pop/16/4/10.1063/1.3106684
http://aip.metastore.ingenta.com/content/aip/journal/pop/16/4/10.1063/1.3106684
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Normalized growth rate vs for the Compton regime parameters , , , and : Solid line is found by solving Eq. (13), broken line is from Eq. (20), and dotted line is from Eq. (21).

Image of FIG. 2.
FIG. 2.

Normalized growth rate vs for the Raman regime parameters , , , and : Solid line is found by solving Eq. (13) and broken line is from Eq. (20).

Image of FIG. 3.
FIG. 3.

Normalized growth rate vs for the strong pump regime parameters , , , and : Solid line is found by solving Eq. (13) and broken line is from Eq. (20).

Image of FIG. 4.
FIG. 4.

Normalized growth rate vs for different values of momentum spread in Raman parameters , , , and ; found by solving Eq. (13).

Image of FIG. 5.
FIG. 5.

Normalized maximum growth rate vs for Raman parameters , , , and ; shows the cold beam limit, × shows the transition to the warm beam, and growth rate becomes half of the cold beam value at ○.

Image of FIG. 6.
FIG. 6.

Normalized maximum growth rate vs for the Compton parameters , , , and ; shows the cold beam limit, × shows the transition to the warm beam, shows the warm beam limit by computer simulation, and growth rate becomes half of the cold beam at ○.

Image of FIG. 7.
FIG. 7.

Normalized maximum growth rate vs for the Raman parameters , , and ; shows the cold beam limit, at and growth rate starts to fall, at ○ and ○○ growth rate is half of the cold beam, and × and ×× are the warm beam limit: double marks , ○○, and ×× are from Ref. 3.

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/content/aip/journal/pop/16/4/10.1063/1.3106684
2009-04-21
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Stability properties of free-electron laser in Raman regime with thermal electron beam
http://aip.metastore.ingenta.com/content/aip/journal/pop/16/4/10.1063/1.3106684
10.1063/1.3106684
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