First Demonstration of Ionization Cooling by the Muon Ionization Cooling Experiment

M. Bogomilov, C. Booth, P. Owens, N. Collomb, I. Mullacrane, C. Pidcott, Y. Kuno, A. Oates, P. Kyberd, R. Mazza, R. Gamet, C. White, D. Summers, D. Sanders, M. Popovic, P. Snopok, N. Jovančević, K. Dumbell, C. Brown, C. Hunt, D. Kaplan, V. Palladino, K. Long, S. Gourlay, G. Chatzitheodoridis, J. Nebrensky, A. Dobbs, M. Savic, A. Demello, J. Nikolov, C. Whyte, F. Chignoli, P. Cooke, G. Hanson, S. Wilbur, A. Nichols, M. Chung, C. Rogers, J. Boehm, H. Witte, R. Preece, C. Macwaters, S. Griffiths, T. Stanley, A. Muir, J. Martyniak, S. Middleton, J. Govans, P. Warburton, R. Tsenov, C. Sung, S. Prestemon, P. Jurj, A. Bross, J. Nugent, T. Lord, P. Hodgson, A. Wilson, R. Gardener, L. Cremaldi, J. Lagrange, S. Virostek, J. R. Greis, A. Kurup, M. Hills, F. Drielsma, D. Maletic, T. Luo, G. Stokes, K. Ronald, T. Bradshaw, S. Ricciardi, M. Vretenar, R. Asfandiyarov, A. Sato, P. Rubinov, E. Overton, M. Tucker, R. Bertoni, V. Blackmore, L. Tortora, A. Blondel, G. Charnley, H. Sakamoto, A. Gallagher, T. Mohayai, C. Heidt
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Abstract

High-brightness muon beams of energy comparable to those produced by state-of-the-art electron, proton and ion accelerators have yet to be realised. Such beams have the potential to carry the search for new phenomena in lepton-antilepton collisions to extremely high energy and also to provide uniquely well-characterised neutrino beams. A muon beam may be created through the decay of pions produced in the interaction of a proton beam with a target. To produce a high-brightness beam from such a source requires that the phase space volume occupied by the muons be reduced (cooled). Ionization cooling is the novel technique by which it is proposed to cool the beam. The Muon Ionization Cooling Experiment collaboration has constructed a section of an ionization cooling cell and used it to provide the first demonstration of ionization cooling. We present these ground-breaking measurements.
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用μ子电离冷却实验首次证明了电离冷却
与最先进的电子、质子和离子加速器产生的能量相当的高亮度μ介子束尚未实现。这样的光束有可能将轻子-反轻子碰撞的新现象的搜索带到极高的能量,并提供独特的、特征良好的中微子束。通过质子束与靶相互作用产生的介子衰变,可以产生介子束。要从这样的光源产生高亮度光束,需要减少(冷却)介子所占据的相空间体积。离子化冷却是提出的一种冷却束流的新技术。μ子电离冷却实验合作已经构建了一个电离冷却细胞的一部分,并用它来提供电离冷却的第一个演示。我们提出这些突破性的测量结果。
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