Abstract

The Oide effect considers the synchrotron radiation in the final focusing quadrupole, and it sets a lower limit on the vertical beam size at the interaction point, particularly relevant for high-energy linear colliders. The theory of the Oide effect was derived considering only the second moment of the radiation in the focusing plane of the magnet. This article addresses the theoretical calculation of the radiation effect on the beam size considering the first and second moments of the radiation and both focusing and defocusing planes of the quadrupole. The effect for a Gaussian beam is referred to as 2D-Oide; however, an alternative beam size figure is given that could represent better the effect on the minimum achievable ${\ensuremath{\beta}}_{y}^{*}$. The CLIC 3 TeV final quadrupole (QD0) and beam parameters are used to compare the theoretical results from the Oide effect and the 2D-Oide effect with particle tracking in placet. The 2D-Oide effect is demonstrated to be important, as it increases by 17% the contribution to the beam size. Further insight into the aberrations induced by the synchrotron radiation opens the possibility to partially correct the 2D-Oide effect with octupole magnets. A beam size reduction of 4% is achieved in the simplest configuration, using a single octupole.

Highlights

  • Synchrotron radiation in a focusing quadrupole magnet of length L and gradient k, schematically represented in Fig. 1, changes the energy of the particle and modifies the focusing effect

  • The Oide effect considers the synchrotron radiation in the final focusing quadrupole, and it sets a lower limit on the vertical beam size at the interaction point, relevant for high-energy linear colliders

  • The best result obtained with the octupole corrector is a vertical beam size reduction by ð−4.3 Æ 0.5Þ%, equivalent to a 6% reduction in the Oide effect contribution to beam size, which agrees with the removal of the cubic component on the beam size

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Summary

INTRODUCTION

Synchrotron radiation in a focusing quadrupole magnet of length L and gradient k, schematically represented in Fig. 1, changes the energy of the particle and modifies the focusing effect. Synchrotron radiation in a focusing quadrupole magnet of length L and gradient k, schematically represented, changes the energy of the particle and modifies the focusing effect This results in a limit on the minimum beam size at the interaction point (IP) located at a distance là from the quadrupole. In order to gain an understanding for the relevant case of CLIC at 3 TeV, Sec. II is dedicated to the theoretical derivation of the effect of radiation including the horizontal beam size and optics lattice parameters (2D-Oide) and comparing results with particle tracking. II is dedicated to the theoretical derivation of the effect of radiation including the horizontal beam size and optics lattice parameters (2D-Oide) and comparing results with particle tracking This leads to a possible way to mitigate the effect, alternative to enlarging QD0, consisting in removing the correlation at the IP via normal octupole magnets. Oide effect beam size contribution for CLIC 3 TeV design parameters. (a) Total beam size normalized to the designed linear beam size as a function of the quad length for the minimum focusing k and the current QD0. (b) k in the two previous cases

Analytical derivation
Simulation
Mitigating the impact on the beam size by a nonlinear corrector scheme
CONCLUSIONS
Full Text
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