Bunching phase evolution of short-pulse FEL oscillator system
We studied numerically the short-pulse FEL oscillator system using properly defined bunching phase θ B and Ψ B . In stable operation, we have found that the optical field “locks” the phase to π/2 at the trailing edge, which gives the maximum gain. Moreover, electrons can be detrapped from ponderomot...
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Published in: | Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Vol. 445; no. 1; pp. 116 - 123 |
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Main Authors: | , , |
Format: | Journal Article |
Language: | English |
Published: |
Elsevier B.V
01-05-2000
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Subjects: | |
Online Access: | Get full text |
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Summary: | We studied numerically the short-pulse FEL oscillator system using properly defined bunching phase
θ
B
and
Ψ
B
. In stable operation, we have found that the optical field “locks” the phase to π/2 at the trailing edge, which gives the maximum gain. Moreover, electrons can be detrapped from ponderomotive bucket due to the spatial variation of the optical field, and this detrapping effect is a major cause of the limit cycle oscillation of the system. The `bump’ of the output power during the amplification usually exists at the near-perfect cavity synchronism regime, which can be explained as the change of the matching condition between electron micropulse and optical pulse. |
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ISSN: | 0168-9002 1872-9576 |
DOI: | 10.1016/S0168-9002(00)00125-X |