Demonstration of cooling by the Muon Ionization Cooling Experiment
- Bogomilov, M.
- Tsenov, R.
- Vankova-Kirilova, G.
- Song, Y. P.
- Tang, J. Y.
- Li, Z. H.
- Bertoni, R.
- Bonesini, M.
- Chignoli, F.
- Mazza, R.
- Palladino, V.
- de Bari, A.
- Orestano, D.
- Tortora, L.
- Kuno, Y.
- Sakamoto, H.
- Sato, A.
- Ishimoto, S.
- Chung, M.
- Sung, C. K.
- Filthaut, F.
- Jokovic, D.
- Maletic, D.
- Savic, M.
- Jovancevic, N.
- Nikolov, J.
- Vretenar, M.
- Ramberger, S.
- Asfandiyarov, R.
- Blondel, A.
- Drielsma, F.
- Karadzhov, Y.
- Boyd, S.
- Greis, J. R.
- Lord, T.
- Pidcott, C.
- Taylor, I.
- Charnley, G.
- Collomb, N.
- Dumbell, K.
- Gallagher, A.
- Grant, A.
- Griffiths, S.
- Hartnett, T.
- Martlew, B.
- Moss, A.
- Muir, A.
- Mullacrane, I.
- Oates, A.
- Owens, P.
- Stokes, G.
- Warburton, P.
- White, C.
- Adams, D.
- Bayliss, V.
- Boehm, J.
- Bradshaw, T. W.
- Brown, C.
- Courthold, M.
- Govans, J.
- Hills, M.
- Lagrange, J.-B.
- Macwaters, C.
- Nichols, A.
- Preece, R.
- Ricciardi, S.
- Rogers, C.
- Stanley, T.
- Tarrant, J.
- Tucker, M.
- Watson, S.
- Wilson, A.
- Bayes, R.
- Nugent, J.C.
- Soler, F. J. P.
- Chatzitheodoridis, G. T.
- Dick, A. J.
- Ronald, K.
- Whyte, C. G.
- Young, A. R.
- Gamet, R.
- Cooke, P.
- Blackmore, V. J.
- Colling, D.
- Dobbs, A.
- Dornan, P.
- Franchini, P.
- Hunt, C.
- Jurj, P. B.
- Kurup, A.
- Long, K.
- Martyniak, J.
- Middleton, S.
- Pasternak, J.
- Uchida, M. A.
- Cobb, J. H.
- Booth, C. N.
- Hodgson, P.
- Langlands, J.
- Overton, E.
- Pec, V.
- Smith, P. J.
- Wilbur, S.
- Ellis, M.
- Gardener, R. B. S.
- Kyberd, P.
- Nebrensky, J. J.
- DeMello, A.
- Gourlay, S.
- Lambert, A.
- Li, D.
- Luo, T.
- Prestemon, S.
- Virostek, S.
- Palmer, M.
- Witte, H.
- Adey, D.
- Bross, A. D.
- Bowring, D.
- Liu, A.
- Neuffer, D.
- Popovic, M.
- Rubinov, P.
- Freemire, B.
- Hanlet, P.
- Kaplan, D. M.
- Mohayai, T. A.
- Rajaram, D.
- Snopok, P.
- Torun, Y.
- Cremaldi, L. M.
- Sanders, D. A.
- Summers, D. J.
- Coney, L. R.
- Hanson, G. G.
- Heidt, C.
- collaboration, MICE
DOIAbstract
The use of accelerated beams of electrons, protons or ions has furthered the development of nearly every scientific discipline. However, high-energy muon beams of equivalent quality have not yet been delivered. Muon beams can be created through the decay of pions produced by the interaction of a proton beam with a target. Such 'tertiary' beams have much lower brightness than those created by accelerating electrons, protons or ions. High-brightness muon beams comparable to those produced by state-of-the-art electron, proton and ion accelerators could facilitate the study of lepton-antilepton collisions at extremely high energies and provide well characterized neutrino beams1-6. Such muon beams could be realized using ionization cooling, whic...
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