Abstract

Here we describe some relationships between cavity shape and fields on and near its surface that can be used for better understanding of the surface field properties. The problem of accelerating cavity optimization lies in the search of the shape with minimal peak magnetic or electric field for a given acceleration rate. This problem became especially important due to widespread use of superconducting cavities where the maximal magnetic field appeared to have a hard limit. The peak magnetic field can be lowered if one can increase the peak electric field but the electric field is also limited because of field emission. The problem of minimal losses in a cavity is very close to the problem of minimal peak magnetic field, though it is not the same, it relates to the lowest average field for a given acceleration rate. The field configuration on the cavity surface is also responsible for the phenomenon of multipactor. Cavities with these properties---minimal peak fields, minimal losses, and absence of multipactor---are found within the set of elliptic cavities. Further improvement of these properties is possible if we step out of the limits of elliptic shapes.

Highlights

  • The commonly used superconducting cavity shape for high β values is a result of evolution from a pillbox rf cavity with the beam tubes added and rounded walls—to decrease the peak electric field—to a shape consisting of elliptic arcs to prevent multipacting [1,2]

  • The relationship between the parameters of these arcs is a subject of cavity optimization in search of the best consistency between maxima of the surface electric and magnetic fields that defines the maximal acceleration achievable in the cavity

  • We present some relationships found for the fields in an elliptic cavity defined by its shape

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Summary

INTRODUCTION

The commonly used superconducting cavity shape for high β values is a result of evolution from a pillbox rf cavity with the beam tubes added and rounded walls—to decrease the peak electric field—to a shape consisting of elliptic arcs to prevent multipacting [1,2]. The relationship between the parameters of these arcs is a subject of cavity optimization in search of the best consistency between maxima of the surface electric and magnetic fields that defines the maximal acceleration achievable in the cavity. We present some relationships found for the fields in an elliptic cavity defined by its shape These relations can be used for any axially symmetric cavity with a smooth inner surface and would be useful in search of an other than elliptic shape with minimal peak magnetic field, or, more definitely, with minimal value of Hpk=Eacc for given values of Epk=Eacc, wall slope angle α, and the. These expansions of fields near the equator were used for multipactor calculations [7]

ELLIPTIC GEOMETRY AND SURFACE FIELDS
USAGE OF MAXWELL’S EQUATIONS
FIELDS ON THE SURFACE OF A PILLBOX CAVITY
TAYLOR EXPANSION OF THE FIELDS NEAR THE CAVITY IRIS
R2aRc þ
Electric field on the iris
Magnetic field in the equator area
CONSISTENCY OF FIELDS ON THE UPPER ARC WITH ITS SHAPE
Findings
VIII. CONCLUSION
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