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Precision Measurement of Muon Capture on the Proton “ Cap experiment” - + p + n Petersburg Nuclear Physics Institute (PNPI), Gatchina,Russia Paul Scherrer Institut, PSI, Villigen, Switzerland University of California, Berkeley, UCB and LBNL, USA University of Illinois, Urbana-Champaign, USA Universite Catholique de Louvain, Belgium TU Munich,Garching, Germany Boston University, USA University of Kentucky, USA @ PSI Cap Steven Clayton APS April Meeting May 2, 2004
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Muon Capture and g P ChPT OP (ms -1 ) gPgP RMC Cap expected error Saclay exp theory OMC Saclay update from Gorringe & Fearing precise QCD (ChPT prediction) no overlap theory & OMC & RMC
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experimental challenges e+ e + - p ( ) + n p (Rich) physics effects Interpretation: where does capture occur ? Critical because of strong spin dependence of V-A interaction Background: Wall stops and diffusion Transfer to impurities p+Z Z +p Rate and statistics (BR = 10 -3 ) SR effect for + TT SS pp pp pp ortho para F=0 F=1 J=1 J=0 n+ Cap
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Cap Experimental Strategy I Cap New idea: active target of ultra-pure H 2 gas 10 bar measure + and - S = 1/ - - 1/ +, to 10 -5 eSC e “Lifetime” or “Disappearance” Method Our experiment observes e + and e – decay products. Muon capture reduces the μ – lifetime compared to the μ + lifetime by 0.15% ! High precision measurement of the lifetime difference: TPC ePC1 ePC2 log(counts) time μ+μ+ μ – 10 10 events
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Cap Experimental Strategy II Physics Unambiguous interpretation At low density (1% LH 2 ) mostly capture from p(F=0) atomic state. Clean muon stop definition: Wall stops and diffusion eliminated by 3-D muon tracking In situ gas impurity control (c Z <10 -8, c d <10 -6 ) hydrogen chambers bakeable to 150 C, continuous purification TPC monitors impurities in-situ 10 -8 sensitivity with gas chromatograph + SR: calibrated with transverse field 70 G Statistics 10 10 decay events: Complementary analysis methods Cap pp pp P pp O time ( s ) 100% LH 2 1 % LH 2 pp P pp O pp
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Cap Experimental Setup Key ideas: active target of ultra-pure H 2 gas 10 bar for muons, separate large tracking detector for electrons. Cap Scintillator (t = 0) Wire Chambers Time Projection Chamber (target) Wire Chambers Hodoscope μ Muon Detectors Electron Detectors e
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The Time Projection Chamber tracks muon stops in 3D. p --
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Event Display Stop Stop Distribution Beam ViewSide View Beam ViewSide View
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Impurity Monitoring Stop Impurity Capture Beam ViewSide View Impurity Capture Yield vs. Time Yield per Stop Time
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Cap Time Projection Chamber in Clean Room
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Cap Assembly: March → August Data-Taking: September → mid-October. commissioning / first physics 2003 Run
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Time Spectra 2003
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Cap Status and Plans Cap 2003 Commissioning Run: achieved high purity ~10 9 - events in 2 weeks analysis of data to get S to ~4% by end of 2004 2004 Upgrades: install 2 nd electron wire chamber install gas recirculation system The Fall 2004 Production Run should collect 10 10 + events and 10 10 - events, giving S to ~1%. Cap Collaboration Website: www.npl.uiuc.edu/exp/mucapture/ Steven Clayton smclayto@uiuc.edu
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Muon Capture and g P ChPT OP (ms -1 ) gPgP RMC Cap expected error Saclay exp theory OMC Saclay update from Gorringe & Fearing TRIUMF exp, 2004 precise QCD (ChPT prediction) no overlap theory & OMC & RMC
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Cap experimental setup Key ideas: active target of ultra-pure H 2 gas 10 bar for muons, separate large tracking detector for electrons. Cap SC (t = 0) PC1 PC2 TPC ePC2 ePC1eSC (Hodoscope) μ Muon Detectors Electron Detectors e
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Event Display y direction (drift time) x direction z direction Anodes Strips y direction (drift time) z direction Stop Distribution Stop
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Impurity Monitoring y direction (drift time) x direction z direction Anodes Strips Stop Impurity Capture
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