PPT-MICE & novel muon /neutrino beams

1 The basis of the potential of muon beams Muon mass 200 m e m m 01 m p Muon decay n e n m Precisely known energy spectrum Energy frontier No brem beam. 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 = . Context: Muon Collider and Neutrino Factory. 1997. : Colin . Johnson argued . that the next step after the ACOL antiproton production target should be a mercury jet target. . [U. Miss. Workshop, Jan 1997; my introduction to Muon Collider . 1. May, 5th 2015. Vertical/. Floor. . big. . beams. . connection. with. an angle . stiffener. Neutrino. 2. May, 5th 2015. Vertical/. Floor. . big. . beams. . connection. with. an angle . stiffener. 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 . Muon. Source. K. McDonald. Princeton U.. . (December . 5. , 2014). MAP Winter Meeting. SLAC. The Target System Concept. A . M. uon. Collider needs . muon. beams of both signs.. A Neutrino Factory based on neutrinos from . 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. Context: Muon Collider and Neutrino Factory. 1997. : Colin . Johnson argued . that the next step after the ACOL antiproton production target should be a mercury jet target. . [U. Miss. Workshop, Jan 1997; my introduction to Muon Collider . Cioli Barazandeh, Angel . Gutarra-leon. and Walerian Majewski. Mentor: . Walerian. . Majewski. , Department of Physics . Northern Virginia Community College, Annandale, VA . Experiments. Hello, and welcome to my Presentation!. 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. 28 March 2018. Perspectives on Laser H. -. Manipulation. Exciting times for Proton and Neutrino Beams. J-PARC. Nearly 500 kW T2K beam (& 1 MW capable neutron beam). Plans to go to 1.3 MW with upgrades. 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 !. Past and Present. Art McDonald. Queen’s University. And. SNOLAB. 1940’s to 1960’s:. Neutrino oscillations were proposed by . Pontecorvo. in 1957 motivated by initial reports of measurements by Davis with a Chlorine detector at a reactor. At that point, the transitions being considered were electron neutrino to electron anti-neutrino.. 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??. Colliders. 26. th. and 27. th. January 2022 . Neutrino Radiation Assessment and Mitigation. C. Ahdida, C. Carli. , . N. Guilhaudin, G. . Lacerda, . A. Lechner, G. Lerner, Y. Robert, D. Schulte, K. Skoufaris.