001389144 001__ 1389144
001389144 003__ SzGeCERN
001389144 005__ 20231201051635.0
001389144 0248_ $$aoai:cds.cern.ch:1389144$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
001389144 035__ $$9arXiv$$aoai:arXiv.org:1110.1813
001389144 035__ $$9Inspire$$a931198
001389144 037__ $$9arXiv$$aarXiv:1110.1813$$cphysics.acc-ph
001389144 037__ $$aFERMILAB-CONF-11-934-AD
001389144 041__ $$aeng
001389144 100__ $$aBravar, U.$$uNew Hampshire U.
001389144 245__ $$aMICE: the Muon Ionization Cooling Experiment. Step I: First Measurement of Emittance with Particle Physics Detectors
001389144 269__ $$c11 Oct 2011
001389144 260__ $$c2011
001389144 300__ $$a9 p
001389144 500__ $$aPreliminary entry
001389144 500__ $$9arXiv$$aProceedings of the DPF-2011 Conference, Providence, RI, August 8-13, 2011
001389144 520__ $$aThe Muon Ionization Cooling Experiment (MICE) is a strategic R&D project intended to demonstrate the only practical solution to providing high brilliance beams necessary for a neutrino factory or muon collider. MICE is under development at the Rutherford Appleton Laboratory (RAL) in the United Kingdom. It comprises a dedicated beamline to generate a range of input muon emittances and momenta, with time-of-flight and Cherenkov detectors to ensure a pure muon beam. The emittance of the incoming beam will be measured in the upstream magnetic spectrometer with a scintillating fiber tracker. A cooling cell will then follow, alternating energy loss in Liquid Hydrogen (LH2) absorbers to RF cavity acceleration. A second spectrometer, identical to the first, and a second muon identification system will measure the outgoing emittance. In the 2010 run at RAL the muon beamline and most detectors were fully commissioned and a first measurement of the emittance of the muon beam with particle physics (time-of-flight) detectors was performed. The analysis of these data was recently completed and is discussed in this paper. Future steps for MICE, where beam emittance and emittance reduction (cooling) are to be measured with greater accuracy, are also presented.
001389144 520__ $$9arXiv$$aThe Muon Ionization Cooling Experiment (MICE) is a strategic R&D project intended to demonstrate the only practical solution to providing high brilliance beams necessary for a neutrino factory or muon collider. MICE is under development at the Rutherford Appleton Laboratory (RAL) in the United Kingdom. It comprises a dedicated beamline to generate a range of input muon emittances and momenta, with time-of-flight and Cherenkov detectors to ensure a pure muon beam. The emittance of the incoming beam will be measured in the upstream magnetic spectrometer with a scintillating fiber tracker. A cooling cell will then follow, alternating energy loss in Liquid Hydrogen (LH2) absorbers to RF cavity acceleration. A second spectrometer, identical to the first, and a second muon identification system will measure the outgoing emittance. In the 2010 run at RAL the muon beamline and most detectors were fully commissioned and a first measurement of the emittance of the muon beam with particle physics (time-of-flight) detectors was performed. The analysis of these data was recently completed and is discussed in this paper. Future steps for MICE, where beam emittance and emittance reduction (cooling) are to be measured with greater accuracy, are also presented.
001389144 540__ $$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
001389144 595__ $$aLANL EDS
001389144 65017 $$2arXiv$$aAccelerators and Storage Rings
001389144 65027 $$2arXiv$$aParticle Physics - Experiment
001389144 690C_ $$aPREPRINT
001389144 690C_ $$aCERN
001389144 695__ $$9LANL EDS$$aphysics.acc-ph
001389144 695__ $$9LANL EDS$$ahep-ex
001389144 700__ $$aBogomilov, M.
001389144 700__ $$aKaradzhov, Y.
001389144 700__ $$aKolev, D.
001389144 700__ $$aRussinov, I.
001389144 700__ $$aTsenov, R.
001389144 700__ $$aWang, L.
001389144 700__ $$aXu, F.Y.
001389144 700__ $$aZheng, S.X.
001389144 700__ $$aBertoni, R.
001389144 700__ $$aBonesini, M.
001389144 700__ $$aMazza, R.
001389144 700__ $$aPalladino, V.
001389144 700__ $$aCecchet, G.
001389144 700__ $$ade Bari, A.
001389144 700__ $$aCapponi, M.
001389144 700__ $$aIaciofano, A.
001389144 700__ $$aOrestano, D.
001389144 700__ $$aPastore, F.
001389144 700__ $$aTortora, L.
001389144 700__ $$aIshimoto, S.
001389144 700__ $$aSuzuki, S.
001389144 700__ $$aYoshimura, K.
001389144 700__ $$aMori, Y.
001389144 700__ $$aKuno, Y.
001389144 700__ $$aSakamoto, H.
001389144 700__ $$aSato, A.
001389144 700__ $$aYano, T.
001389144 700__ $$aYoshida, M.
001389144 700__ $$aFilthaut, F.
001389144 700__ $$aVretenar, M.$$uCERN
001389144 700__ $$aRamberger, S.
001389144 700__ $$aBlondel, A.
001389144 700__ $$aCadoux, F.
001389144 700__ $$aMasciocchi, F.
001389144 700__ $$aGraulich, J.S.
001389144 700__ $$aVerguilov, V.
001389144 700__ $$aWisting, H.
001389144 700__ $$aPetitjean, C.
001389144 700__ $$aSeviour, R.
001389144 700__ $$aEllis, M.
001389144 700__ $$aKyberd, P.
001389144 700__ $$aLittlefield, M.
001389144 700__ $$aNebrensky, J.J.
001389144 700__ $$aForrest, D.
001389144 700__ $$aSoler, F.J.P.
001389144 700__ $$aWalaron, K.$$iINSPIRE-00170872
001389144 700__ $$aCooke, P.
001389144 700__ $$aGamet, R.
001389144 700__ $$aAlecou, A.
001389144 700__ $$aApollonio, M.
001389144 700__ $$aBarber, G.
001389144 700__ $$aDobbs, A.$$iINSPIRE-00334793
001389144 700__ $$aDornan, P.
001389144 700__ $$aFish, A.$$iINSPIRE-00037759
001389144 700__ $$aHare, R.
001389144 700__ $$aJamdagni, A.
001389144 700__ $$aKasey, V.$$iINSPIRE-00350630
001389144 700__ $$aKhaleeq, M.$$iINSPIRE-00350646
001389144 700__ $$aLong, K.
001389144 700__ $$aPasternak, J.
001389144 700__ $$aSakamoto, H.
001389144 700__ $$aSashalmi, T.
001389144 700__ $$aBlackmore, V.
001389144 700__ $$aCobb, J.
001389144 700__ $$aLau, W.
001389144 700__ $$aRayner, M.
001389144 700__ $$aTunnell, C.D.$$iINSPIRE-00166263
001389144 700__ $$aWitte, H.$$iINSPIRE-00015871
001389144 700__ $$aYang, S.
001389144 700__ $$aAlexander, J.
001389144 700__ $$aCharnley, G.
001389144 700__ $$aGriffiths, S.
001389144 700__ $$aMartlew, B.
001389144 700__ $$aMoss, A.
001389144 700__ $$aMullacrane, I.
001389144 700__ $$aOats, A.
001389144 700__ $$aYork, S.
001389144 700__ $$aApsimon, R.
001389144 700__ $$aAlexander, R.J.
001389144 700__ $$aBarclay, P.
001389144 700__ $$aBaynham, D.E.
001389144 700__ $$aBradshaw, T.W.
001389144 700__ $$aCourthold, M.
001389144 700__ $$aHayler, R.Edgecock T.
001389144 700__ $$aHills, M.
001389144 700__ $$aJones, T.
001389144 700__ $$aMcNubbin, N.
001389144 700__ $$aMurray, W.J.
001389144 700__ $$aNelson, C.
001389144 700__ $$aNicholls, A.
001389144 700__ $$aNorton, P.R.
001389144 700__ $$aPrior, C.
001389144 700__ $$aRochford, J.H.
001389144 700__ $$aRogers, C.$$iINSPIRE-00016069
001389144 700__ $$aSpensley, W.
001389144 700__ $$aTilley, K.
001389144 700__ $$aBooth, C.N.
001389144 700__ $$aHodgson, P.
001389144 700__ $$aNicholson, R.
001389144 700__ $$aOverton, E.
001389144 700__ $$aRobinson, M.$$iINSPIRE-00346160
001389144 700__ $$aSmith, P.
001389144 700__ $$aAdey, D.
001389144 700__ $$aBack, J.
001389144 700__ $$aBoyd, S.
001389144 700__ $$aHarrison, P.
001389144 700__ $$aNorem, J.
001389144 700__ $$aBross, A.D.$$uFermilab
001389144 700__ $$aGeer, S.$$uFermilab
001389144 700__ $$aMoretti, A.$$uFermilab
001389144 700__ $$aNeuffer, D.$$uFermilab
001389144 700__ $$aPopovic, M.$$uFermilab
001389144 700__ $$aQian, Z.$$uFermilab
001389144 700__ $$aRaja, R.$$uFermilab
001389144 700__ $$aStefanski, R.$$uFermilab
001389144 700__ $$aCummings, M.A.C.$$uMUONS Inc., Batavia
001389144 700__ $$aRoberts, T.J.$$uMUONS Inc., Batavia
001389144 700__ $$aDeMello, A.$$uLBL, Berkeley
001389144 700__ $$aGreen, M.A.$$iINSPIRE-00336683$$uLBL, Berkeley
001389144 700__ $$aLi, D.$$uLBL, Berkeley
001389144 700__ $$aSessler, A.M.$$uLBL, Berkeley
001389144 700__ $$aVirostek, S.$$uLBL, Berkeley
001389144 700__ $$aZisman, M.S.$$uLBL, Berkeley
001389144 700__ $$aFreemire, B.$$uIIT, Chicago
001389144 700__ $$aHanlet, P.$$uIIT, Chicago
001389144 700__ $$aHuang, D.
001389144 700__ $$aKafka, G.$$uIIT, Chicago
001389144 700__ $$aKaplan, D.M.$$uIIT, Chicago
001389144 700__ $$aSnopok, P.
001389144 700__ $$aTorun, Y.$$uIIT, Chicago
001389144 700__ $$aOnel, Y.$$uIowa U.
001389144 700__ $$aCline, D.$$uUCLA
001389144 700__ $$aLee, K.$$uUCLA
001389144 700__ $$aFukui, Y.$$uUCLA
001389144 700__ $$aYang, X.$$uUCLA
001389144 700__ $$aRimmer, R.A.$$uJefferson Lab
001389144 700__ $$aCremaldi, L.M.$$uMississippi U.
001389144 700__ $$aHart, T.L.$$uMississippi U.
001389144 700__ $$aSummers, D.J.$$uMississippi U.
001389144 700__ $$aConey, L.$$iINSPIRE-00074206$$uUC, Riverside
001389144 700__ $$aFletcher, R.$$uUC, Riverside
001389144 700__ $$aHanson, G.G.$$uUC, Riverside
001389144 700__ $$aHeidt, C.$$iINSPIRE-00347825$$uUC, Riverside
001389144 700__ $$aGallardo, J.$$uBrookhaven
001389144 700__ $$aKahn, S.$$uBrookhaven
001389144 700__ $$aKirk, H.$$uBrookhaven
001389144 700__ $$aPalmer, R.B.$$uBrookhaven
001389144 773__ $$aC11-08-09
001389144 8564_ $$uhttps://lss.fnal.gov/archive/2011/conf/fermilab-conf-11-934-ad.pdf$$yFermilab Library Server
001389144 8564_ $$82321392$$s1183758$$uhttp://cds.cern.ch/record/1389144/files/arXiv:1110.1813.pdf
001389144 8564_ $$82497391$$s1159527$$uhttp://cds.cern.ch/record/1389144/files/3a781fd050826a54bd887d46cb3febe2.pdf$$yFulltext
001389144 916__ $$sn$$w201141
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001389144 980__ $$aPREPRINT
001389144 980__ $$aConferencePaper