Muon Collider Design
R. Palmer, A. Sessler, A. Skrinsky, A. Tollestrup, A. Baltz, S. Caspi, P. Chen, W-H. Cheng, Y. Cho, D. Cline, E. Courant, R. Fernow, J. Gallardo, A. Garren, H. Gordon, M. Green, R. Gupta, A. Hershcovitch, C. Johnstone, S. Kahn, H. Kirk, T. Kycia, Y. Lee, D. Lissauer, A. Luccio, A. McInturff, F. Mills, N. Mokhov, G. Morgan, D. Neuffer, K-Y. Ng, R. Noble, J. Norem, B. Norum, K. Oide, Z. Parsa, V. Polychronakos, M. Popovic, P. Rehak, T. Roser, R. Rossmanith, R. Scanlan, L. Schachinger, G. Silvestrov, I. Stumer, D. Summers, M. Syphers, H. Takahashi, Y. Torun, D. Trbojevic, W. Turner, A. Van Ginneken, T. Vsevolozhskaya, R. Weggel, E. Willen, W. Willis, D. Winn, J. Wurtele, Y. Zhao
Abstract
Muon Colliders have unique technical and physics advantages and disadvantages when compared with both hadron and electron machines. They should thus be regarded as complementary. Parameters are given of 4 TeV and 0.5 TeV high luminosity μ+ μ- colliders, and of a 0.5 TeV lower luminosity demonstration machine. We discuss the various systems in such muon colliders, starting from the proton accelerator needed to generate the muons and proceeding through muon cooling, acceleration and storage in a collider ring. Detector background, polarization, and nonstandard operating conditions are discussed.
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