2001
DOI: 10.1103/physreve.65.016505
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Field analysis of a dielectric-loaded rectangular waveguide accelerating structure

Abstract: In this paper, we present a detailed analysis of the modes of a dielectric-loaded rectangular waveguide accelerating structure. In general, the acceleration field in a synchronous acceleration mode is non-uniform in the two transverse dimensions. However, we could use an array of these structures rotated alternatively by 90 degrees to get a focusing-defocusing force continuously as a simple FODO lattice, while maintaining uniform energy gain. The expressions of characteristic parameters such as R/Q, group velo… Show more

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Cited by 74 publications
(66 citation statements)
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“…This is not obvious for the solution obtained by the impedance method [25,26] and requires additional analysis and proof.…”
Section: Introductionmentioning
confidence: 99%
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“…This is not obvious for the solution obtained by the impedance method [25,26] and requires additional analysis and proof.…”
Section: Introductionmentioning
confidence: 99%
“…Finally, (i) the proposed method does not require any assumptions on the form of the beam's Coulomb field (in contrast to the impedance method [25,26], where it is often assumed that the field of the beam is essentially flat, an assumption that is valid only at ultrarelativistic energies); (ii) we also did not use the mode decomposition for the problem formulation and its subsequent solution; the mode series obtained as a solution emerges in a natural way as a result of solving the problem; (iii) as a consequence of (ii), and the use of the transverse operator formalism the series of modes of the solution is uniformly convergent. This is not obvious for the solution obtained by the impedance method [25,26] and requires additional analysis and proof.…”
Section: Introductionmentioning
confidence: 99%
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“…Therefore, the design of the DLW structures must compromise between a small transverse size to maximize the intensity of the wakefield, and a longer interaction length to maximize the energy gain of the test charge. An appealing solution consists of using flat electron beams passing through slab-geometry DLWs [14,[23][24][25]. This possibility has become more attractive since the recent advances toward generating flat beams directly in photoinjectors [26,27].…”
Section: Introductionmentioning
confidence: 99%