Precision Measurement of Singlet mp Capture in a Hydrogen TPC

Slides:



Advertisements
Similar presentations
A.Vorobyov on behalf of MuCap collaboration Determination of the nucleon’s pseudoscalar form factor in the MuCap experiment HSQCD 2014 Gatchina
Advertisements

Muon Capture on the Proton Final results from the MuCap experiment Muon Capture on the Proton Final results from the MuCap experiment gPgP Peter Winter.
Commissioning the PHENIX RPC Forward Trigger Upgrade Michael Daugherity Abilene Christian University for the PHENIX Collaboration.
Precision Measurement of Muon Capture on the Proton “  Cap experiment”  - + p   + n  PSI Supported by Paul Scherrer.
1 Peter Kammel for the MuSun Collaboration Muon Capture on the Deuteron The MuSun Experiment BV39, Feb 21, 08.
2 July 2004Journée DPNC 2004 FAST: A precision measurement of muon lifetime. Chiara Casella FAST collaboration: A.Barczyk (1), J. Berdugo (2), J. Casaus.
Precision Muon Physics Group muon capture on proton  - + p   + n  to 1 % muon capture on proton  - + p   + n  to 1 % Nucleon form factors, chiral.
Precision Measurement of Muon Capture on the Proton “  Cap experiment”  - + p   + n Petersburg Nuclear Physics Institute (PNPI), Gatchina,Russia Paul.
The Design of MINER  A Howard Budd University of Rochester August, 2004.
New Precision Determination of g p and G F, the MuXperiments at PSI Bernhard Lauss University of Berkeley on behalf of the MuCAP and MuLAN.
Muon Capture as a Probe of the Nucleon’s Axial Structure – the  Cap Experiment Peter Kammel University of Illinois at Urbana-Champaign
Peter Kammel University of Illinois at Urbana-Champaign MuCap Collaboration V.A. Andreev,
1 Measurement of the Rate of Muon Capture in Hydrogen Gas and Determination of the Proton’s Pseudoscalar Coupling Steven Clayton Dissertation Talk June.
MuCap High-Precision Measurement of Muon Capture on the Proton BVR35 Progress report presented by Claude Petitjean, PSI 12 Febuary 2004
Measurement of B (D + →μ + ν μ ) and the Pseudoscalar Decay Constant f D at CLEO István Dankó Rensselaer Polytechnic Institute representing the CLEO Collaboration.
MuCap: From first results to final precision on determining g P Brendan Kiburg 2008 APS April Meeting April 12 th, 2008.
Data Analysis and Present Status of the MuCap Experiment Steven Clayton* University of Illinois *Present address: LANL Outline: 1)Experimental overview.
Status of DRIFT II Ed Daw representing the DRIFT collaboration: Univ. of Sheffield, Univ. of Edinburgh, Occidental College, Univ. of New Mexico Overview.
Precision Muon Capture on the Proton and Very Light Nuclei 1 Peter Kammel Department of Physics and Center for Experimental Nuclear Physics and Astrophysics,
2 1/March/2015 日本物理学会大70回年次大会@早稲田大学 東大ICEPP 内山雄祐 他 MEG II collaboration.
Monte Carlo Comparison of RPCs and Liquid Scintillator R. Ray 5/14/04  RPCs with 1-dimensional readout (generated by RR) and liquid scintillator with.
Precision Muon Capture at PSI 1 Peter Kammel Department of Physics and Center for Experimental Nuclear Physics and Astrophysics, University of Washington.
MEG positron spectrometer Oleg Kiselev, PSI on behalf of MEG collaboration.
EPECUR – Investigation of narrow baryon resonances Konovalova Elena St. Petersburg Nuclear Physics Institute (PNPI) with collaboration Institute of Theoretical.
Status of E391a Search for K L    decay G.Y.Lim IPNS, 32nd ICHEP 19 th August 2004 Beijing.
Muon PSI Peter Winter University of Washington gPgP L 1A / d R.
Peter Kammel First Results from the New Muon Lifetime Experiments at PSI GFGF gPgP L 1A MuCap “MuSun” project MuLan.
NanoPHYS’12 – December 17-19, 2012 K. Nakano, S. Miyasaka, K. Nagai and S. Obata (Department of Physics, Tokyo Institute of Technology) Drift Chambers.
TPC R&D status in Japan T. Isobe, H. Hamagaki, K. Ozawa, and M. Inuzuka Center for Nuclear Study, University of Tokyo Contents 1.Development of a prototype.
Malte Hildebrandt, PSIMEG - Review Meeting / 1   e  Drift Chambers Charge Division Test Chamber Testsetup for Cosmics Chamber Construction.
Performance of a Large-Area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System Vallary Bhopatkar M. Hohlmann, M. Phipps, J. Twigger,
A Silicon vertex tracker prototype for CBM Material for the FP6 Design application.
Muon Capture in Hydrogen and Deuterium EXA08 int. conference on exotic atoms & related topics Vienna Sept presentation by Claude Petitjean representing.
22 September 2005 Haw05 1  (1405) photoproduction at SPring-8/LEPS H. Fujimura, Kyoto University Kyoto University, Japan K. Imai, M. Niiyama Research.
Unblinding the MuCap experiment the final results of μp capture rate Λ S and of electro-weak coupling constant g P LTP Seminar April 23, 2012 Claude Petitjean.
Muon Capture on the Proton: First Physics Results from the MuCap Experiment Steven Clayton University of Illinois Urbana Champaign
Abstract Beam Test of a Large-area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System V. Bhopatkar, M. Hohlmann, M. Phipps, J. Twigger,
CP violation in B decays: prospects for LHCb Werner Ruckstuhl, NIKHEF, 3 July 1998.
Beam Test of a Large-Area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System Vallary Bhopatkar M. Hohlmann, M. Phipps, J. Twigger, A.
Concept Design for LBNF Far detector (LAr single phase)
ПРЕЦИЗИОННОЕ ИЗМЕРЕНИЕ СКОРОСТИ ЗАХВАТА МЮОНА В ВОДОРОДЕ И ОПРЕДЕЛЕНИЕ ПСЕВДОСКАЛЯРНОГО ФОРМ ФАКТОРА ПРОТОНА g P PNPI participants in MuCAP collaboration*)
Muon Capture: Status and Prospects 1 Peter Kammel Department of Physics and Center for Experimental Nuclear Physics and Astrophysics, University of Washington.
NSS2006Shengli Huang1 The Time of Flight Detector Upgrade at PHENIX Shengli Huang PHENIX Collaboration Outlines: 1.Physics motivations 2.Multi-gap Resistive.
The MuCap experiment – final results on μp capture rate Λ S and pseudoscalar coupling g P INPC 2013 Firence Italia June 2 - 7, 2013 Claude Petitjean on.
Quark Matter 2002, July 18-24, Nantes, France Dimuon Production from Au-Au Collisions at Ming Xiong Liu Los Alamos National Laboratory (for the PHENIX.
Trigger & Tracking detector for CMS
1 Peter Kammel Muon Capture and Basic Solar Neutrino Reactions The New MuSun Experiment Muon Capture and Basic Solar.
R&D activities on a double phase pure Argon THGEM-TPC A. Badertscher, A. Curioni, L. Knecht, D. Lussi, A. Marchionni, G. Natterer, P. Otiougova, F. Resnati,
FEE for TPC MPD__NICA JINR
High-Precision Measurement of Muon Capture on the Proton
Test Beam Request for the Semi-Digital Hadronic Calorimeter
First operation of a double phase pure liquid Argon THGEM-TPC
Study of Hypernuclei with Heavy Ion Beams (HypHI) at GSI Shizu Minami GSI, Germany on behalf of HypHI collaboration Introduction Phase 0 experiment R.
A. Badertscher, L. Knecht, D. Lussi, A. Marchionni, G. Natterer, P
AT-TPC project at NSCL/MSU
CMS muon detectors and muon system performance
The MuCap experiment: A measurement of
Silicon Pixel Detector for the PHENIX experiment at the BNL RHIC
Muon Capture on the Deuteron The MuSun Experiment
First results from the MuLan and MuCap experiments
High Precision Measurement of Muon Capture on the Proton
Multigap Resistive Plate Chambers (MRPC)
Toward the final design of a TPC for the ILD detector
VEPP-2000 plans for the study of the nucleon form factors
Muon Detector Jiawen ZHANG 16 September 2002.
Search for f-N Bound State in Jefferson Lab Hall-B
Pre-installation Tests of the LHCb Muon Chambers
Design of active-target TPC
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
The LHCb Level 1 trigger LHC Symposium, October 27, 2001
Presentation transcript:

Precision Measurement of Singlet mp Capture in a Hydrogen TPC V.A. Andreev, D.V. Balin, A.A. Fetisov, V.A. Ganzha, V.I. Jatsoura, A.G. Krivshich, E.M. Maev, O.E. Maev, G.E. Petrov, S. Sadetsky, G.N. Schapkin, G.G. Semenchuk, M. Soroka, A.A. Vorobyov, N.I. Voropaev Petersburg Nuclear Physics Institute (PNPI), Gatchina,Russia P.U. Dick, A. Dijksman, J. Egger, W.D. Herold, V. Markushin, C. Petitjean, R. Schmidt, W. Schoeps Paul Scherrer Institut, PSI, Villigen, Switzerland T.A. Case, K.M. Crowe, P. Kammel University of California, Berkeley, UCB and LBNL, USA J. Deutsch, J. Govaerts, R. Prieels Universite Catholique de Louvain Belgium F.J. Hartmann Technische Universitaet Muenchen,Garching, Germany introduction experimental progress towards final experiment outlook

rate LS (from mp(F=0) state) goal - + p  m+ n rate LS (from mp(F=0) state) LS to 1% gp to 7% precision method pure protium TPC @ 10 bar as active target unambiguous interpretation clean m stop definition gas impurity control high statistics measure -/m+ lifetime in hydrogen to 10 ppm LS = 1/- - 1/+ LS ~1.5x10-3 l0 physics test hadronic symmetries of Standard Model : QCD tests, chiral symmetry breaking, pseudoscalar formfactor gP(q2 = - 0.88 m2m) electro-weak symmetries of lepton-quark interaction m-e universality, additional interactions at quark-lepton level J. Govaerts, nucl-th/0004056 (2000). Nucl Phys A, in press

theory: LS = 688.4±3.8 s-1 Ja = Va - Aa nucleon charged current at q2= - 0.88 mm2 Ja = Va - Aa Va= gV(q2) ga + igM(q2) sab qb/2M Aa= gA(q2) ga g5 + igP(q2) qa/m g5 gA(0)=1.2670(35) q2 dependence from quasielastic n scattering CVC: gV(0)=1, gM(0)=mp-mn-1 q2 dependence from e scatt. nucleon weak CC formfactors gV(q2) = 0.9755(5) gA(q2) = 1.245(3) gM(q2) = 3.5821(25) gP(q2) = 8.44(23) gP(q2) = 8.21(09) PCAC heavy baryon chiral perturbation theory: accurate QCD prediction, precise expt’l test mssing nm n p m- gpNN Fp

main experimental challenges Physics effects Interpretation At low density (1% LH2) mostly capture from mp(F=0) atomic state. Wall stops and diffusion. Stop volume determined by tracking, transfer, diffusion suppressed. Transfer to impurities. (cZ<10-8, cd<10-7) . TPC monitors nuclear recoils from m+Z  Z’+n+n and transfer to deuterium. Continuous purification/monitoring system system. mSR effect for m+. Tranverse field ~70G. LT LS m ppm pm Lortho Lpara F=0 F=1 J=1 J=0 lOP Time distortions due to detector effects Self correlation Two event correlations additional background terms correlated losses (“double kill”) time dependent efficiency ? Statistics 1010 statistics. Different analysis methods. Complementary: Tracking of m-e vertices of several m’s to overcome pile-up. Pile-up free data sample. m decay at all stages, l0

Experimental progress Jan 97 proposal R-97-05 presented at BVR, start phase 1: design, test basic detector system Aug 97 progress report (systematics, chamber prototypes) Dec 98 1st test run prototype TPC+4 MWPCs new DAQ, analog readout (12 channels) Mar 99 continuation test run digital readout, new TDC 400, 100 channels Dec 99 2nd test run TPC amd 6 MWPC, m and e internal/ext tracking full digital readout all channels, 500 channels. Mar 00 continuation test run upgraded DAQ, event selection and compression DAQ with 3 thresholds Mar 00 gas system development gas purification and chromatography at 0.01 ppm protium production Apr 00 start phase 2: design high purity detector system

Prototype Oct 99 Gatchina dimension: 30 x 15 x 10 cm3 gas gain 5000 (e) drift velocity (cm/s) 0.6 @ 2 kV/cm voltage (kV) cathode -30 cathodes strip - 6.5 anodes 0 material diam(mm) pitch(mm) gap(mm) cathode stainless/W 50 1 3.5 anode W 25 4 3.5 Gatchina

Digital Readout two thresholds for TPC (electrons, muons) custom made (Berkeley/PSI) deadtime less TDCs high bandwidth DAQ to processor farm, VME-64, VX works readout of contiguous (ms) time regions to provide complete history information

muon tracking Dt Dz=8cm

PU free time spectra m - m + 12 ms 12 ms xe+l0t m stop in fiducial volume e after m time (bin width 200ns)

PU free, external e tracking

Impurities effect on lifetime of 0.01 ppm Z>1 1. ppm D ~0.01 ppm required or 0.1 ppm if measured & corrected detection in TPC impurity capture m+Z  Z’+n+n

Gas system gas handling and purity analysis system developed. 0.01 ppm purity and sensitivity achieved. 3 LN2 traps, zeolite absorber, compressor production 60L/h gas chromatograph A) commercial hydrogen, 1L, O2~0.1ppm, N2~0.2ppm B) after cleaning, 30L, O2<0.001ppm, N2~0.02ppm on site analysis of TPC gas no special materials/ purification of TPC prototype

m transfer to deuterium, diffusion mp+d  md + p  pmd  m(5.3MeV)+3He(0.2KeV) Ramsauer Townsend minimum in md + p scattering at 1.6 eV mp md pmd m+He

Concept final experiment Option 1 i) m tracked with scint, MWPC & TPC ii) e tracked with MWPC/scint. combination external to hydrogen vessel iii) samples of competing background processes recorded with selective trigger (3rd threshold) Dead-time free data taking of event class I) and ii) Data includes pile-up and pile-up free events for complementary analysis. 1010 pile-up free m-e (m+,m-) in 2 months Option 2 Hermetic geometry with all MWPC inside hydrogen vessel. e tracked with MWPC combination inside the hydrogen vessel No windows, very small multiple scattering. Pad TPC During next months we will evaluate options based on analysis of test runs, Monte Carlo test of materials and procedures, without/with beam to define final set-up.

Technical design all components inside H2 low outgasing, bakeable to 120 C wires W 4.5 ppm/K cathode frame Kovar 4.8 ppm/K anode frame ceramic/Pyrex 6./3. ppm/K external detectors inner detector: chamber 3 SINDRUM I f =38.4cm, L = 58cm outer detector: chamber or scint. array a’la mLAN DAQ upgrade with 2-4 VME CPUs CAEN tdc’s for MWPC readout High vacuum& gas handling integrate present purification system non mechanical circulation system based on zeolite absobers at LN2 temperature (400atmL/h) present (new) protium system <1ppm, 0.1 level needs careful study

study final design by MC

Summary and outlook phase 1: basically finished optimize set-up & detector elements develop subsystems: electronics high speed DAQ gas purification, analysis study physics characteristics phase 2: started develop ultra-clean techniques (det., recirculation) increase solid angle of external detectors construction final detector system integration further generation Muon on Request : LS gP present proposal 1% 7% with MORE 0.3% 2% tentative schedule technical report within next 6-12 months commissioning & start of production 2001-2002 collaboration

Statistics

Gas System

diffusion

external tracking