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Premium member Presentation Transcript Slide1: MuCap High-Precision Measurement of Muon Capture on the Proton BVR35 Progress report presented by Claude Petitjean, PSI 12 Febuary 2004 http://www.npl.uiuc.edu/exp/mucapture/ mMuCap Experiment: MuCap Experiment experimental goal principle of measurement apparatus time projection chamber (TPC) data from run in fall 2003 some results milestones reached in 2003 upgrades for run in fall 2004 Beam request 2004 Slide3: MuCap collaboration V.A. Andreev, A.A. Fetisov, V.A. Ganzha, V.I. Jatsoura, A.G. Krivshich, E.M. Maev, O.E. Maev, G.E. Petrov, G.N. Schapkin, G.G. Semenchuk, M. Soroka, A.A. Vorobyov Petersburg Nuclear Physics Institute (PNPI), Gatchina 188350, Russia P.U. Dick, A. Dijksman, J. Egger, D. Fahrni, M. Hildebrandt, A. Hofer, L. Meier, C. Petitjean, R. Schmidt Paul Scherrer Institute, PSI, CH-5232 Villigen, Switzerland T.I. Banks, T.A. Case, K.M. Crowe, S.J. Freedman, F.E. Gray, B. Lauss University of California Berkeley, UCB and LBNL, Berkeley, CA 94720, USA K.D. Chitwood, S.M. Clayton, P.T. Debevec, D. W. Hertzog, P. Kammel, B. Kiburg, R. McNabb, F. Mulhauser, C. J. G. Onderwater, C. Ozben, C.C. Polly, A. Sharp, D. Webber University of Illinois at Urbana-Champaign, Urbana, IL 61801, USA L. Bonnet, J. Deutsch, J. Govaerts, D. Michotte, R. Prieels Université Catholique de Louvain, B-1348 Louvain-La-Neuve, Belgium R. M. Carey. J. Paley Boston University, Boston, MA 02215, USA T. Gorringe, M. Ojha, P. Zolnierzcuk University of Kentucky, Lexington, KY 40506, USA F.J. Hartmann Technische Universität München, D-85747 Garching, Germany mCapExperimental goal: Experimental goal measure the rate Λs of muon capture on the proton to 1% precision. Muon capture is a semileptonic weak interaction process, and occurs predominantly from the hyperfine singlet atomic bound state. problem of previous experiments: problem of previous experiments LT LS m ppm ppm pm pm Lortho Lpara F=0 F=1 J=1 J=0 lOP n+n n+n n+n interpretation of rate LS due to formation of ppμ molecules in lq hydrogen and badly known rate lOP of ortho-para transitionsMuon Capture and gP: Muon Capture and gP ChPT lOP (ms-1) gP RMC mCap proposed Saclay exp theory OMC Saclay update from Gorringe & Fearing interpretation of gP vs lOP ---------o--------- New TRIUMF expExperimental Technique: Experimental Technique “Lifetime” Method For μ–, muon capture competes with muon decay: This rate decreases the observed μ– lifetime from the vacuum lifetime, which we measure separately with μ+ : Thus we need 10 ppm measurements of the μ+/- lifetimes or a statistics of at least 1010 for both μ-decaysExperimental Technique: Experimental Technique “Lifetime” or “Disappearance” Method Since our experiment can only observe e+ and e– decay products, muon capture produces a small downward deflection of the μ– lifetime curve from the μ+ “vacuum” lifetime curve : The capture rate is easily calculated from the measured lifetimes: log(counts) time μ+ μ – Technical tasks of MuCap experiment: Technical tasks of MuCap experiment ultra-clean 10-bar hydrogen gas target 0.01 ppm Z>1 impurities deuterium depleted hydrogen („protium“) < 1 ppm deuterium 100% stop identification no wall stops TPC clean electron identification & tracking 2 cylindrical wire chambers unique μ e decay assignment μ-stop – e-vertex matching high data rate 30 kHz μ stops high statistics > 1010 events for μ+ and μ- μSR under control for μ+ 50-100 Gauss magnetic field tasks goals to be reachedExperimental Setup – Apparatus: Experimental Setup – Apparatus μSC μPC1 μPC2 TPC ePC2 ePC1 eSC (Hodoscope) μ beam Muon Detectors Electron Detectors • e-detectors cover 75% of 4πSlide11: assembly/tests: March-Aug 2003 data-taking: Sept-Oct 2003 Slide12: Ucathodes = 5-6 kV E = 2 kV/cm - vdrift = 0.5 cm/μs sensitive volume (12 x 15 x 30) cm3 TPC design drawing with glass frames and ceramic structure bakeable to 130 CSlide15: Online display of μ beam, μ stops in TPC and e in ePC1 ePC1/eSC(phi,z)event display of muon stops & electrons: event display of muon stops & electronsevent display of μ stop + impurity capture: event display of μ stop + impurity capturedevelopment of impurities during the 2 good data weeks: development of impurities during the 2 good data weeks full scale 1 ppmSlide20: summed decay time spectra showing pile-up suppressionSlide21: μ – decay time spectra of 1 week with clean protium filling Slide22: MuCap 2003: exponential fits to each eSC counter pairSlide23: MuCap 2003: μSR enhanced fit of μ+ decay time spectramilestones 2003: milestones 2003 protium production with < 0.5 ppm deuterium ultra-clean protium gas filling (< 0.1 ppm impurities) – after installation of a new Palladium filter new TPC@4.8 kV stable operation (perfect μ stop detector!) full e detector consisting of ePC1 and eSC new frontend electronics for ePC1 new compressor electronics for deadtime free ePC1 data collection new DAQ running with 4 MB/s data rate (80% duty cycle) new μSR magnet with ~50 Gauss field new slow control system full electronics for TPC, wire chambers and plastic counters collimated muon beam injection system analysis software in mature development upgrades for 2004: upgrades for 2004 protium: maintain < 0.5 ppm deuterium & < 0.1 ppm Z>1 impurities new gas circulation, cleaning & diagnostics (Gatchina) e-detector: include new ePC2 ( vertex tracking) tune TPC to 5.5 kV ( online control of μd diffusion) new 0.5 mm Beryllium window ( increase good μ stops x 2) μ-detectors: new outside μPC1&2 ( reduce μ-absorption/range-tails) μ-beam: new tune in πE3 area ( < 3% momentum spread) new spare TPC from Gatchina ( >6 kV to see e tracks) upgrade DAQ for larger data flow ( ~100% duty cycle) upgrade μSR magnet with Alu coils ( reduce scattering of e) new online data analysis goal for 2004: collect a significant part of 1010 pileup-protected good μ-decays for μ+ and μ-Slide28: protium gas circulation and purifying system (Gatchina)Slide29: MCstudy of μ stop distributions for various beam windowsSlide30: MuCap experiment: time plans of upgrades for 2004 runMuCap experiment: beam request for 2004: MuCap experiment: beam request for 2004 In 2004 we hope to approach closely the goal formulated in the proposal: a measurement of the μp singlet capture rate to ± 1% accuracy To accomplish this goal, we need area πE3 for the following activities: setup of beamline with el.stat. separator, assemble full apparatus and electronics, test all components in the beam: 2 weeks tune new 35 MeV/c muon beam: 1 week test & optimize complete detector with beam: 1 week data production towards 1010 good μ- & μ+ decays: 2 x 2.5 weeks contingency for beam losses or other failures 1 week we request 10 weeks in area πE3 (preferably in Oct-Dec 2004, at the end of the 2004 production cycle) You do not have the permission to view this presentation. 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bvr35 Me_I Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 21 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: October 12, 2007 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: MuCap High-Precision Measurement of Muon Capture on the Proton BVR35 Progress report presented by Claude Petitjean, PSI 12 Febuary 2004 http://www.npl.uiuc.edu/exp/mucapture/ mMuCap Experiment: MuCap Experiment experimental goal principle of measurement apparatus time projection chamber (TPC) data from run in fall 2003 some results milestones reached in 2003 upgrades for run in fall 2004 Beam request 2004 Slide3: MuCap collaboration V.A. Andreev, A.A. Fetisov, V.A. Ganzha, V.I. Jatsoura, A.G. Krivshich, E.M. Maev, O.E. Maev, G.E. Petrov, G.N. Schapkin, G.G. Semenchuk, M. Soroka, A.A. Vorobyov Petersburg Nuclear Physics Institute (PNPI), Gatchina 188350, Russia P.U. Dick, A. Dijksman, J. Egger, D. Fahrni, M. Hildebrandt, A. Hofer, L. Meier, C. Petitjean, R. Schmidt Paul Scherrer Institute, PSI, CH-5232 Villigen, Switzerland T.I. Banks, T.A. Case, K.M. Crowe, S.J. Freedman, F.E. Gray, B. Lauss University of California Berkeley, UCB and LBNL, Berkeley, CA 94720, USA K.D. Chitwood, S.M. Clayton, P.T. Debevec, D. W. Hertzog, P. Kammel, B. Kiburg, R. McNabb, F. Mulhauser, C. J. G. Onderwater, C. Ozben, C.C. Polly, A. Sharp, D. Webber University of Illinois at Urbana-Champaign, Urbana, IL 61801, USA L. Bonnet, J. Deutsch, J. Govaerts, D. Michotte, R. Prieels Université Catholique de Louvain, B-1348 Louvain-La-Neuve, Belgium R. M. Carey. J. Paley Boston University, Boston, MA 02215, USA T. Gorringe, M. Ojha, P. Zolnierzcuk University of Kentucky, Lexington, KY 40506, USA F.J. Hartmann Technische Universität München, D-85747 Garching, Germany mCapExperimental goal: Experimental goal measure the rate Λs of muon capture on the proton to 1% precision. Muon capture is a semileptonic weak interaction process, and occurs predominantly from the hyperfine singlet atomic bound state. problem of previous experiments: problem of previous experiments LT LS m ppm ppm pm pm Lortho Lpara F=0 F=1 J=1 J=0 lOP n+n n+n n+n interpretation of rate LS due to formation of ppμ molecules in lq hydrogen and badly known rate lOP of ortho-para transitionsMuon Capture and gP: Muon Capture and gP ChPT lOP (ms-1) gP RMC mCap proposed Saclay exp theory OMC Saclay update from Gorringe & Fearing interpretation of gP vs lOP ---------o--------- New TRIUMF expExperimental Technique: Experimental Technique “Lifetime” Method For μ–, muon capture competes with muon decay: This rate decreases the observed μ– lifetime from the vacuum lifetime, which we measure separately with μ+ : Thus we need 10 ppm measurements of the μ+/- lifetimes or a statistics of at least 1010 for both μ-decaysExperimental Technique: Experimental Technique “Lifetime” or “Disappearance” Method Since our experiment can only observe e+ and e– decay products, muon capture produces a small downward deflection of the μ– lifetime curve from the μ+ “vacuum” lifetime curve : The capture rate is easily calculated from the measured lifetimes: log(counts) time μ+ μ – Technical tasks of MuCap experiment: Technical tasks of MuCap experiment ultra-clean 10-bar hydrogen gas target 0.01 ppm Z>1 impurities deuterium depleted hydrogen („protium“) < 1 ppm deuterium 100% stop identification no wall stops TPC clean electron identification & tracking 2 cylindrical wire chambers unique μ e decay assignment μ-stop – e-vertex matching high data rate 30 kHz μ stops high statistics > 1010 events for μ+ and μ- μSR under control for μ+ 50-100 Gauss magnetic field tasks goals to be reachedExperimental Setup – Apparatus: Experimental Setup – Apparatus μSC μPC1 μPC2 TPC ePC2 ePC1 eSC (Hodoscope) μ beam Muon Detectors Electron Detectors • e-detectors cover 75% of 4πSlide11: assembly/tests: March-Aug 2003 data-taking: Sept-Oct 2003 Slide12: Ucathodes = 5-6 kV E = 2 kV/cm - vdrift = 0.5 cm/μs sensitive volume (12 x 15 x 30) cm3 TPC design drawing with glass frames and ceramic structure bakeable to 130 CSlide15: Online display of μ beam, μ stops in TPC and e in ePC1 ePC1/eSC(phi,z)event display of muon stops & electrons: event display of muon stops & electronsevent display of μ stop + impurity capture: event display of μ stop + impurity capturedevelopment of impurities during the 2 good data weeks: development of impurities during the 2 good data weeks full scale 1 ppmSlide20: summed decay time spectra showing pile-up suppressionSlide21: μ – decay time spectra of 1 week with clean protium filling Slide22: MuCap 2003: exponential fits to each eSC counter pairSlide23: MuCap 2003: μSR enhanced fit of μ+ decay time spectramilestones 2003: milestones 2003 protium production with < 0.5 ppm deuterium ultra-clean protium gas filling (< 0.1 ppm impurities) – after installation of a new Palladium filter new TPC@4.8 kV stable operation (perfect μ stop detector!) full e detector consisting of ePC1 and eSC new frontend electronics for ePC1 new compressor electronics for deadtime free ePC1 data collection new DAQ running with 4 MB/s data rate (80% duty cycle) new μSR magnet with ~50 Gauss field new slow control system full electronics for TPC, wire chambers and plastic counters collimated muon beam injection system analysis software in mature development upgrades for 2004: upgrades for 2004 protium: maintain < 0.5 ppm deuterium & < 0.1 ppm Z>1 impurities new gas circulation, cleaning & diagnostics (Gatchina) e-detector: include new ePC2 ( vertex tracking) tune TPC to 5.5 kV ( online control of μd diffusion) new 0.5 mm Beryllium window ( increase good μ stops x 2) μ-detectors: new outside μPC1&2 ( reduce μ-absorption/range-tails) μ-beam: new tune in πE3 area ( < 3% momentum spread) new spare TPC from Gatchina ( >6 kV to see e tracks) upgrade DAQ for larger data flow ( ~100% duty cycle) upgrade μSR magnet with Alu coils ( reduce scattering of e) new online data analysis goal for 2004: collect a significant part of 1010 pileup-protected good μ-decays for μ+ and μ-Slide28: protium gas circulation and purifying system (Gatchina)Slide29: MCstudy of μ stop distributions for various beam windowsSlide30: MuCap experiment: time plans of upgrades for 2004 runMuCap experiment: beam request for 2004: MuCap experiment: beam request for 2004 In 2004 we hope to approach closely the goal formulated in the proposal: a measurement of the μp singlet capture rate to ± 1% accuracy To accomplish this goal, we need area πE3 for the following activities: setup of beamline with el.stat. separator, assemble full apparatus and electronics, test all components in the beam: 2 weeks tune new 35 MeV/c muon beam: 1 week test & optimize complete detector with beam: 1 week data production towards 1010 good μ- & μ+ decays: 2 x 2.5 weeks contingency for beam losses or other failures 1 week we request 10 weeks in area πE3 (preferably in Oct-Dec 2004, at the end of the 2004 production cycle)