THE RF SYSTEM FOR THE MICE EXPERIMENT

THE RF SYSTEM FOR THE MICE EXPERIMENT
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DOI:
10.22323/1.226.0124
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发表时间:
2013-12
期刊:
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影响因子:
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通讯作者:
K. Ronald;C. Whyte;A. Dick;A. Moss;A. Grant;C. White;P. Corlett;T. Stanley;D. Li;A. Demello;S. Virostek;A. Moretti;R. Pasquinelli;D. Peterson;R. Schultz;J. Volk;Y. Torun;P. Hanlet;K. Long;J. Pasternak;C. Hunt;D. Summers;T. Luo;Pete Smith
K. Ronald;C. Whyte;A. Dick;A. Moss;A. Grant;C. White;P. Corlett;T. Stanley;D. Li;A. Demello;S. Virostek;A. Moretti;R. Pasquinelli;D. Peterson;R. Schultz;J. Volk;Y. Torun;P. Hanlet;K. Long;J. Pasternak;C. Hunt;D. Summers;T. Luo;Pete Smith
中科院分区:
其他
文献类型:
--
作者:
K. Ronald;C. Whyte;A. Dick;A. Moss;A. Grant;C. White;P. Corlett;T. Stanley;D. Li;A. Demello;S. Virostek;A. Moretti;R. Pasquinelli;D. Peterson;R. Schultz;J. Volk;Y. Torun;P. Hanlet;K. Long;J. Pasternak;C. Hunt;D. Summers;T. Luo;Pete Smith

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国际Muon电离冷却实验(MICE)旨在展示电离冷却的有效性,以减少带电粒子束的相空间足迹,主要是为了允许下一代对撞机和/或中微子工厂随后加速Muon。该实验(以及基于相同原理的任何后续加速器冷却通道)对其射频系统提出了某些不寻常的要求,而对电离冷却过程的精确测量需要特殊的诊断。本文将概述射频系统的主要特点,包括低电平射频控制、功率放大链、分配网络、腔、调谐器和耦合器,所有这些都必须在强磁场环境中工作。还应讨论与其他鼠标诊断相结合的RF诊断,该诊断将允许详细了解在每个单独的Muon过境期间的加速场的幅度和相位。
The International Muon Ionisation Cooling Experiment (MICE) is designed to demonstrate the effectiveness of ionisation cooling to reduce the phase space footprint of a charged particle beam, principally to allow the subsequent acceleration of muons for next generation colliders and/or neutrino factories. The experiment (and indeed any subsequent accelerator cooling channel based on the same principles) poses certain unusual requirements on its RF system, whilst the precision measurement of the ionisation cooling process demands special diagnostics. This paper shall outline the key features of the RF system, including the low level RF control, the power amplifier chain, distribution network, cavities, tuners and couplers, all of which must operate in a high magnetic field environment. The RF diagnostics which, in conjunction with the other MICE diagnostics, shall allow detailed knowledge of the amplitude and phase of the acceleration field during the transit of each individual muon shall also be discussed.