Abstract

The six-dimensional beam-beam interaction as developed in 1992 by Hirata, Moshammer, and Ruggiero has been extended to include linear coupled motion and an arbitrary crossing plane. The technique of symplectic mapping in the six-dimensional phase space, called synchrobeam mapping, is applied to investigate the beam-beam kick within a solenoid. A linear beam-beam model including coupling is discussed in detail, also in the framework of a six-dimensional symplectic dispersion formalism.

Highlights

  • The beam-beam interaction is studied in storage rings, using the formalism developed by Hirata, Moshammer, and Ruggiero [synchrobeam mapping (SBM) and a Lorentz boost transforming the collision with a crossing angle to a head-on collision]

  • In this approach the strong bunch is split longitudinally into several slices, where each slice is described by an electrostatic potential of the form

  • It allows one to include the bunch length effect at the collision point and the energy variation caused by the electric field of the opposite bunch

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Summary

INTRODUCTION

The beam-beam interaction is studied in storage rings, using the formalism developed by Hirata, Moshammer, and Ruggiero [synchrobeam mapping (SBM) and a Lorentz boost transforming the collision with a crossing angle to a head-on collision]. In this approach the strong bunch is split longitudinally into several slices, where each slice is described by an electrostatic potential of the form. It allows one to include the bunch length effect at the collision point and the energy variation caused by the electric field of the opposite bunch This mapping is formulated only for head-on collision, but Hirata has shown that a crossing angle can be eliminated by a Lorentz boost [2]. The 6D beam-beam formalism has been incorporated in the tracking programs MAD [3] and SIXTRACK [4]

The electromagnetic field due to a tilted bunch
Lorentz boost
Arbitrary crossing plane
Full Lorentz boost
SUMMARY
Generating function
Lie series
Integration method
Canonical transformation
D2 D3 D4 0
The eigenvalue spectrum of the orbital revolution matrix
Methods
Full Text
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