PPT-Abstract: The Muon Ionization Cooling Experiment (MICE) is an international effort

muon beam A pair of identical 3m long spectrometer solenoids will provide a 4tesla uniform field region at each end of the cooling channel The emittance of the beam as it enters and exits the cooling channel will be measured within the 400 mm diameter magnet bores The magnets incorporate a threecoil spectrometer magnet section and a twocoil section that matches the solenoid uniform field into the MICE cooling channel The cold mass radiation shield and leads are kept cold by means of a series of twostage . Robert P. . Redwine. Director, Bates Linear Accelerator Center. 12/1/2009. 1. Muon Collider Design Workshop, BNL. MIT Bates Linear Accelerator Center. 12/1/2009. 2. Muon Collider Design Workshop, BNL. Introduction to MICE. After the LHC…. Many open questions in physics:. Gravity & standard model. Matter-antimatter imbalance. Dark matter. Higher energy collisions = . MUON COLLIDER. Neutrino physics = . its application to Ionization Cooling . for a . Muon. Collider. Project 38b-911255. John Keane. Particle Beam Lasers ,INC. Team J. . Kolonka. , R. Palmer, . H.Kirk. , R. . Wegglel. ,. R. . Scanlan. T. Kallman NASA/GSFC. Line emission efficiency across the spectrum. Thermal stability. The broad-band spectrum of active galaxies. ~flat over 6-8 decades. Very different from stars. Most are strong X-ray sources. Alan Bross. N u F a c t 0 9. From . SuperBeams. to Neutrino Factories. Pre-Ramble. Neutrino Factory means different things to different people. Not so much for . SuperBeams. I will be talking about a muon-based Neutrino Factory as opposed to a . C. Booth, P. Hodgson, R. Nicholson, P. J. Smith, Dept. of Physics & Astronomy. University of Sheffield, England.. p.j.smith@sheffield.ac.uk. for PAC09. 1 – The MICE Experiment . 2 - The Target Mechanism. Goldsmith’s Particle Physics Summer School. 21. st. July 2009. Outline. 1.. . Why MICE?. . - a brief overview of the Standard Model. - . n. eutrino . m. asses and oscillations. - the neutrino factory and muon cooling. Non-DC. Electron Beam. Yuhong. Zhang. For the . JLab. -IMP Cooling Collaboration. JLEIC Collaboration Meeting Fall 2016. October 5 to 7, 2016. The . JLab. -IMP Cooling Collaboration . Andrew Hutton, Kevin Jorden, Tom . Heavy Neutral Leptons at the SPS. (CERN-SPSC-2013-024 / SPSC-EOI-010. ). On behalf of:. 1. Theoretical motivation. Discovery of the 126 . GeV. Higgs boson .  . Triumph of the Standard Model. . The SM may work successfully up to Planck scale !. 1. The basis of the potential of . muon. beams. Muon. mass:. 200. . m. e. ~ . m. m. ~ 0.1. . m. p. Muon. decay:. n. e. , . n. m. Precisely known energy spectrum. Energy frontier:. No . brem. -/beam-. Derun Li. Lawrence Berkeley National Laboratory. MICE RF Workshop. Fermilab, June 2, 2014. MICE. MICE RF Workshop, June 2, 2014 (Fermilab), Derun Li, LBNL. Our responsibilities . in . MICE cooling channel:. . . ILC and More Workshop. Lake Como, Italy. . May 16-17, 2013. Why . Muons. ?. What’s so special about . Muons. ?. Muons. are . Heavy. LHC, MAP, and LEMC. David . Neuffer. July 2018. 2. Outline. Next Heavy Lepton Collider . up to ~14 . TeV. in LHC tunnel. Needs muon source. PS or new MW proton . Linac. /storage ring. cooling …. or LEMC??. 1 particle. Phys. Lett. A, 357, No. 2, 120-124 (2006). 138. Yuri F. Orlov, William M. Morse and Yannis K. Semertzidis, Resonance method of electricdipole-moment measurements in storage rings. Phys.