PPT-Beam Instabilities at the ISIS Neutron & Muon Source

Rob Williamson Supervisors Chris Warsop ISIS Ivan Konoplev JAI Contents Introduction ISIS Synchrotron Loss Mechanisms at ISIS Headtail RampD Damping Systems Summary and Plans Introduction. O. . Tarvainen, T. Kalvas, H. Koivisto, J. . Komppula. , R. Kronholm, J. . Laulainen . University. . of . Jyväskylä. . I. . Izotov. , D. . Mansfeld. , V. . . Skalyga. . Institute . of. Applied . 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 . Targetry. 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 . muon. particle physics . programmes. at J-PARC. Mu_01. Satoshi MIHARA. IPNS, KEK. FKPPL-FJPPL workshop, . Yonesei. Univ.. Outline. Introduction. Physics motivation. J-PARC facility. France-Japan collaboration in the COMET experiment at J-PARC. 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 . for high power deuterium beams. Corso di Dottorato in Fisica e Astronomia: ciclo XXX. Seminario di fine primo anno. Andrea . Muraro. Outline. What is ITER . Neutral Beam Injector for ITER (PRIMA). CNESM Principle. 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. X. . Buffat. , L.R. Carver. Overview. No apparent correlation on unstable bunches with emittance or beam intensity.. No correlation of timing of instabilities with . LHCb. polarity.. New work: further study into . V. . Variale*. , B. Skarbo. 2. 1Istituto Nazionale Fisica Nucleare,INFN Sezione di Bari, Italy. 2 . Budcker. Institute of Nuclear Physics, Novosibirsk, Russia. * Vincenzo Variale. Tel.: +39 080 5442344; fax: +39 080 5443190.. 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??. M. Scott Dewey. National Institute of Standards and Technology. Workshop on Next Generation Neutron Lifetime Measurements in the U.S.. How to Measure . τ. n. … .  . “Bottle” Experiments:. Direct Observation of Exponential Decay:. G. Iadarola, L. . Mether. , E. . Métral. , L. Sabato. Introduction. Instability dependence on the bunch intensity. Dipole magnets. Quadrupole magnets. Experimental observations with trains of 12b. Effect of the transverse emittance. muon . science. Adrian Hillier . ISIS . Muon. Group . PASI ‘15 Chicago, Illinois, USA . MUONS:. Versatile probes of magnetic, superconducting, molecular systems. Analogues of protons/hydrogen in semiconductors.