PPT-High-Power Targets for Muon (and Neutrino) Production

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 . Atoms in magnetic field. orbiting electron behaves like current loop . .  magnetic moment . μ. = current x area . interaction energy = . μ. ·B. (both vectors!) = . μ. ·B. . loop current = -. electron, and electron-neutrino have =+1; their anti-particles have =-1; muon, and muon-neutrino have =+1; their anti-particles have THUS, there should be two types of neutrinos: electron-kind and muo 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 . Upgrade Status. P. Campana, . Muon Upgrade . Meeting, . September 3rd, . 2010. . Progress of the work on Muon Upgrade. . Preparation of LOI-Muon. 1. 2. Some work done since our last meeting:. ODE electronics (Caterina et al. – see separate talk). COSMOLOGY. EVIDENCE FOR NEW PHYSICS?. STEEN . HANNESTAD, Aarhus . University. NuHorizons. 2011. n. e. n. m. n. t. Fermion Mass Spectrum. 10. 100. 1. 10. 100. 1. 10. 100. 1. 10. 100. 1. 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 . of a . Muon. Collider or Neutrino Factory. K. McDonald. Princeton U.. . (August . 29, 2014). NuFact’14. U Glasgow. The Target System Concept. A . M. uon. Collider needs . muon. beams of both signs.. 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!. of a . Muon. Collider or Neutrino Factory. K. McDonald. Princeton U.. . (August . 29, 2014). NuFact’14. U Glasgow. The Target System Concept. A . M. uon. Collider needs . muon. beams of both signs.. End. (IPAC13, TUPFI075. ) . H. K. Sayed,. *1. . J.S. Berg. 1. , X. Ding. 2. , . H.G Kirk,. 1. . K.T. McDonald. 3. 1 . Brookhaven National Laboratory, Upton, NY 11953, USA. 2. UCLA, Los Angeles, CA 90095, USA. Outline. Class 1 Atlas Control Room Shifts. Booking. Present Status + Experience+ Feedback. Class . 2 reminder. A. . Polini. & Z. Yan. May 21. th. 2012. Class 1 Control Room . Muon. Shifts. Following Steering and IB discussions in November:. Talk given in the last year. V. . Kaushik. M. King. P. . Klluit. V. . Kouskoura. J.F . Laporte. J. Meyer. N. Orlando. A. . Orraou. P. . Pais. A. . Polini. E. . Pueschel. S. . Rosati. A. . Salvucci. S. . . . ILC and More Workshop. Lake Como, Italy. . May 16-17, 2013. Why . Muons. ?. What’s so special about . Muons. ?. Muons. are . Heavy. 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..