1990
DOI: 10.1088/0022-3727/23/11/001
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Gauss-Laguerre modes in a high-grain FEL

Abstract: A decomposition is made, in axisymmetric Gauss-Laguerre modes, of the bumpy optical beam shape in a high-grain free electron laser. It is shown that waist position and Rayleigh length can be chosen freely over a wide range of values. A method to optimize the choice is given.

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Cited by 11 publications
(5 citation statements)
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“…Thus the number of modes with significant amplitude can be high if the source point is not chosen well. To avoid this problem an optimization algorithm could change the source point per integration step so that the number of modes stays low (Best and Faatz, 1990). Another drawback is the calculation of the source term.…”
Section: Equation Section 8viii Numerical Codesmentioning
confidence: 99%
“…Thus the number of modes with significant amplitude can be high if the source point is not chosen well. To avoid this problem an optimization algorithm could change the source point per integration step so that the number of modes stays low (Best and Faatz, 1990). Another drawback is the calculation of the source term.…”
Section: Equation Section 8viii Numerical Codesmentioning
confidence: 99%
“…In the simulation, the equation of motion is described using an axis-symmetric beam field Aðx; zÞ decomposed into Gauss-Laguerre modes 26) as…”
Section: The Modelmentioning
confidence: 99%
“…By assuming both beams have the same transverse cross-section are obtained the second equalities of Eqs. (8) and (9) in terms of the beam currents. The coupling of the lower energy electrons to both the fundamental and harmonic fields is seen in Eq.…”
Section: The Modelmentioning
confidence: 99%
“…Equation (6) demonstrates that the harmonic field has two driving sources: the lower-and the higherenergy electron beams. In the simulation, the equation of motion is described using an axis-symmetric beam field A(x,z) decomposed into Gauss-Laguerre modes [9] as…”
Section: The Modelmentioning
confidence: 99%