Abstract

Recently, a new method for calculating the Cherenkov field acting on a point-like electron bunch passing through longitudinally homogeneous structures lined with arbitrary slowdown layers was proposed, where the formalism was obtained though consideration of a general integral relation that allows calculation of the fields at the vicinity of a point-like bunch. It demonstrates that the Cherenkov field at the point of the short relativistic bunch does not depend on the waveguide system material and is a constant for any given transverse dimensions and cross-section shapes of waveguides. With this paper we present a strict derivation of the fields formulas valid at the cross-section of a bunch on the basis of a conformal mapping method. We generalize the results of the previous paper to the case of transversely distributed bunch by deriving a two-dimensional Green function at the cross-section of a bunch. Comparison of the results proving validity of the method is given in the appendix.

Highlights

  • Wakefields excited when very short bunches pass through accelerating structures or other longitudinally extended components of a beam line, are of major concern for linear colliders (ILC [1], CLIC [2]), and FEL (LCLS-II, X-FEL, etc.) [3,4] and other accelerator projects

  • The results were obtained by using formula (31) and found to be in full agreement with those obtained using the mode decomposition method [14,23,24], where dielectric was considered as a retarding layer

  • We provide formulas for the loss factor and transverse Ez field distribution for the case of an elliptical cross section

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Summary

Introduction

Wakefields excited when very short bunches pass through accelerating structures or other longitudinally extended components of a beam line (pipes, collimators, bellows), are of major concern for linear colliders (ILC [1], CLIC [2]), and FEL (LCLS-II, X-FEL, etc.) [3,4] and other accelerator projects. Analysis of the short-range wakefields in the longitudinally extended components, especially in undulator vacuum chambers, is needed to control the energy spread and emittance of the short bunches [5,6]. Theoretical analysis of Cherenkov radiation commonly considers a “short bunch” approach [7,8,9,10].

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