Anomalous free electron laser interaction
Free electron lasers (FELs) are considered, typically, as fast wave devices. The normal FEL interaction satisfies the tuning condition ω≅( k z + k W) V z , where ω and k z are the em-wave angular frequency and longitudinal wave number, respectively, V z is the electron axial speed, and k W is the wi...
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Published in | Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Vol. 483; no. 1; pp. 482 - 487 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
01.05.2002
|
Subjects | |
Online Access | Get full text |
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Summary: | Free electron lasers (FELs) are considered, typically, as fast wave devices. The
normal FEL interaction satisfies the tuning condition
ω≅(
k
z
+
k
W)
V
z
, where
ω and
k
z
are the em-wave angular frequency and longitudinal wave number, respectively,
V
z
is the electron axial speed, and
k
W is the wiggler periodicity. This paper presents an
anomalous FEL interaction, which may occur in slow-wave FELs (i.e. loaded by dielectric or periodic structures). The anomalous FEL effect presented here satisfies the tuning condition
ω≅(
k
z
−
k
W)
V
z
, and it resembles the anomalous effect in slow-wave cyclotron resonance masers. A necessary condition for the anomalous interaction is
ω/
k
z
<
V
z
(i.e., the em-wave phase velocity should be slower than the electron beam). The paper presents a preliminary experimental result demonstrating the anomalous FEL effect in a stripline dielectric-loaded FEL experiment. A linear Pierce equation is applied to describe both the anomalous and normal FELs in the same framework. The paper is concluded with a conceptual discussion. |
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ISSN: | 0168-9002 1872-9576 |
DOI: | 10.1016/S0168-9002(02)00366-2 |