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Emittance dilution due to the betatron mismatch in high-intensity hadron accelerators

机译:高强度强子加速器中电子感应加速器失配导致的发射率稀释

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摘要

The importance of the betatron mismatch between two sections of an accelerator complex was recognized a long time ago. The mismatch together with the filamentation effect will result in a larger diluted beam emittance. However, the influence of the mismatch was underestimated largely in high-intensity hadron synchrotrons in the literature, as the rms emittance is used to represent the dilution. The dilution on the total emittance is significantly larger, which is of more importance in representing the beam loss in proton synchrotrons. This article points out the necessity of using the dilution factor of the total emittance together with the rms emittance in high-intensity hadron accelerators. A proof is given to show that the dilution factor of the rms emittance is the same for any initial beam distribution. The detailed beam distribution after the dilution is discussed for the initial uniform, Gaussian and parabolic distributions, and the numerical simulation results are presented. Examples and discussions about the betatron mismatch in the cases of injection, FODO channel transporting mixed H~- and proton beams, fast-changing periodic focusing systems and proton linacs of a large tune depression are also presented.
机译:很早以前就已经认识到加速器复合体的两个部分之间电子感应加速器不匹配的重要性。失配与灯丝效应一起将导致更大的稀释光束发射率。然而,在文献中,由于均方根发射率用来表示稀释度,因此在高强度强子同步加速器中,失配的影响被大大低估了。对总发射率的稀释明显更大,这对于表示质子同步加速器中的束流损失更为重要。本文指出了在高强度强子加速器中必须使用总发射率的稀释因子以及均方根发射率。给出的证明表明,对于任何初始光束分布,均方根发射率的稀释系数是相同的。讨论了稀释后的初始均匀分布,高斯分布和抛物线分布的详细光束分布,并给出了数值模拟结果。还提供了有关注入情况下电子感应加速器不匹配,FODO通道传输混合的H〜和质子束,快速变化的周期性聚焦系统以及大幅度凹陷的质子直线加速器的示例和讨论。

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