1. A Precision Measurement of the Positive Muon Lifetime Using a Pulsed Muon Beam and the  Lan Detector R.M. Carey, P. Cushman, P.T. Debevec, W. Earle, F.E. Gray, M. Hare, E. Hazen, D.W. Hertzog, I. Kronkvist, J.P. Miller, O. Rind, B.L. Roberts, C.J.G. Onderwater, C.C. Polly, M. Sossong, D.C. Urner, S. Williamson Boston University University of Illinois at Urbana-Champaign University of Minnesota

2. Collaboration Subset of Muon (g-2) Experiment at BNL Responsibilities there include: –electromagnetic calorimeters –traceback wire chambers –waveform digitizers –multi-channel TDCs –flight simulator –custom PMT bases –laser and LED calibration systems –GEANT (and other) simulations –systematic error evaluations –data acquisition –data analysis –(we did not contribute significantly to the magnet design, or field monitoring tasks) We are actively seeking additional collaborators for  Lan, especially in the area of surface muon beam issues,  SR, and local PSI expertise

3. Proposal Summary Determine G F to better than 1 ppm by measuring   10 12 good events “Pulsed” low-energy muon source Symmetric, segmented timing detector “Clocks” Main focus: Systematic Error Control –pileup –gain changes “early-to-late” –backgrounds –errant muons –stray positrons –… Running Plan –many “tests” to establish key systematic error benchmarks –relatively short data collection period... –… which can be repeated, if needed...

4. Present knowledge of    is 18 ppm

5. Classic Lifetime Techniques “1 at a time” –Each muon (or pion) enters target individually with pre- and post-quiet periods. Watch for decay positron and record its time. –Must know incoming efficiency and pileup well –For 10 12, need about 4 x 10 7 sec … several years ! “Multiple Experiments at Once” “  ” beam by time…  Lan muons arrive “at once”, decay into segmented detector by space… FAST pions arrive “DC” into highly segmented timer/tracker

6. “Radioactive” Mode Burst of N muons arrives during accumulation period T acc –Observe muon decays during measuring period of length T meas –No other muons arrive during this time –Get another burst Ideally: –N small; reduces pileup –T acc +T meas ~ 20  sec; cycles fast At PSI with kicker like MORE setup, –cycle frequency ~ 50 kHz –N ~ 10 - 15 works very well Compare with proposed RAL approach –cycle frequency ~ 50 Hz (1000 times slower) –N ~ 2,000 or more and very long run

7. Generic Proposed Setup at PSI separator quads +10 kV 0 -10 kV Kicker Plates After separator, expect e + /  + at few % Kicker sends beam left or right 1.5 x 10 7 beam implies around 15 muons per 1  s accumulation period … and 12 at the start of the measuring period. 20  s Update: Better cycle per PSI kicker HV supply and expt. measuring period Kicker HV Supply quads Desired Extinction 99.9%

8. Beam into Detector Option 1 pmt Helium Bag 1 mm Sulfur disk or other target, (e.g., iron oxide) e+e+ Option 2 pmt Helium Bag e+e+ thin Aluminized mylar wall Active 1 mm thick fiber veto for errant muons Desired Efficiency 99.9%

9. Stopped Muon Distribution in Target

10. Muon Drift through Helium Bag 300 mm

11. Muon Scattering in Scintillator and Window Scintillator 0.2 mm Window 0.15 mm

12. Muon Distribution at Target

13. Tests of muons into target Extinction fraction –easily measured to high accuracy –critical to obtain its time dependence Beam counter efficiency –special test with 2nd small counter behind Note: only time-dependence in these quantities can hurt us Beam distribution on target –use existing thin straw chamber to establish profile Outscattered, errant muons –instrument helium bag to establish this; –also can put in ring around area for permament magnet setup to count number of muons hitting this device

14. Question: What can go wrong? Any “early-to-late” changes in detection capability time shifts gain or threshold shifts Effective change due to residual polarization of muons target choice external B field Pileup Backgrounds Detector and “Clock” must be designed from systematic error issue consideration time counts EeEe threshold time counts i

15. Pileup: When 2 particles are counted as 1* Time-dependent; rate squared pileup fraction ~ e -2t/  To reduce: –Segment DetectorF seg = 180 –Double-hit timing resolution  t = 10 ns –Overlap rejection by energyF dh = 10 At this level we can EASILY correct for it since we will know the factors above very well *Note: if 1 is counted as 2, only changes  2 (if probability is time independent) time counts (our values)

16. Segmentation 180 coincident timing tiles 3D symmetric additional point-symmetry with respect to target for tile pairs Icosahedral geometry: 20 sides Each “SuperTriangle” contains 9 identical tiles Beam enters Target inside Tile segment SuperTriangle  Lan Detector

17. Tile Elements Inner: 6.4 mm thick 300 pe/mip Outer: 3.2 mm thick160 pe/mip Note: actual prototypes, have smoothly tapered cone with round top, etc. e+e+ Note: no real gap between tiles outer inner

18.  t resolution Fast scintillator:e.g. BC418 Fast PMTs:e.g. R6427 Two time measurements per positron 500 MHz waveform digitizer sampling of pulses –Based on our (g-2) experience … can resolve 10 ns with UNequal pulses, and 400 MHz sampling –We are actually hoping to push this number down a bit. 10 ns is not overly optimistic A “similar” MIP pulse in a (g-2) counter with BC404, tube as described, and custom base. RED pulse is a copy displaced by 10 ns

19. F dh Rejection* Normal mode: –single e+ passes through both scintillator tiles leaving “mip” type monoenergetic signal Two with  t < 10 ns –“double” mip signal in both Question: How does this look compared to Landau tails ? –cut in 2-dimensional space –obtain a factor F dh up to 200 ! We are ONLY using F dh of 10 in our calculations to be very conservative *dh = double hit

20. Pulse-height and timing data For (g-2), we have developed timing based on –discriminator/derandomizer/TDCs and –waveform digitizers (WFD) Overwhelming feeling: Only the WFDs matter. Additionally, they provide the pulse height used for the F dh rejection algorithm WFD 500 MHz We plan to use 1 WFD per tile and separate the signals by time. When either fires, the WFD records what is going on in the other….reduces threshold worries

21. Spin Precession Effects change in effective efficiency versus time Asymmetry in detector –mimimized by point-like symmetry –90 tile pairs for (F-B)/(F+B) tests Residual polarization of individual stopped muon –target choice –depolarization high Residual ensemble-averaged polarization after accumulation period –dephasing time T acc by precessing by fast spin relaxation

22. Target Choice Sulfur depolarizes muon spin to about 3% during stopping. –(studies ongoing at PSI now) Good conductors preserve polarization –used for tests of detector symmetry Other targets feature strong B fields, randomly aligned –This reduces = 1/3. e.g., iron oxide –If dynamic changes (fluctuations of field orientations), smaller e.g., certain spin glasses “pause” for spin relaxation

23. A75 G transverse field, rotates  in 1  s Incorporate this small field around target to dephase muons The factor  multiplies the individual residual polarization to yield the net ensemble-averaged polarization  < 0.1 0.05 Dephasing

24. Overall effect Steps to eliminating systematic error due to spin orientation and precession 75 G field 1 ppm error Single , Single tile, No depolarization Add tile pair; asymmetry in pair 2% Add depolarization to 3% (sulfur) Add dephasing factor  = 0.1

25. Proof of factors Step 1: Detector tile symmetry,  –Use Al or Ag which preserves polarization in a 1 at a time mode; no B field –Measure (F-B) i versus time for all tile pairs –Adjust alignment if needed Step 2:Test of Depolarizing targets –Insert Sulfur or other candidate targets and measure  SR signal in a transverse field. What is the residual ? –NOTE: We hope to make use of existing, expert  SR facility and collaborators to do this step early, in year 1 Step 3:Determine Dephasing factor –Al or Ag target –B field at 75 G transverse –Chopped beam, 1  s accumulation period. –Measure residual polarization in single tile –Measure residual polarization in tile combination

26. Gain (threshold) Stability Threshold ~ 2-3 MeV ( thin counters) –(upper 99% of electron energy spectrum) Gain stability to 1% (not hard) – largely determined by number of photoelectrons For N pe > 47, no problem. –Prototypes have N pe > 160

27. Backgrounds Flat (no problem with long measuring period to establish level) –cosmics –accelerator-related room background –must establish that there is no time correlation with chopping Rare Decays May cause “double” hit for one time. No problem because probability is stable, early to late Only effects the overall  2 in a predictable way 1.4% 0.0034%

28. Electronics & DAQ Main development, 500 MHz waveform digitizer –for us, 2nd generation…having built the 400 MHz system for (g-2) (see layout) Basic Idea related to readout… –use FIFO memory in order to readout as you go –Each event consists of approximately 40 WFD samples + timewords –Reduce this number to simpler list using online processor NORMAL EVENT –Spill # –Tile # –Time Inner –Energy Inner –Time Outer –Energy Outer AbNormal EVENT + 10% of all others –Spill # –Tile # –WFD Records to tape

29. DAQ continued Data Volume (an idea only) –10 12 events(a lot!) –normal events (13.5 Tb) –12 bytes/event 9 events per spill »decay positron –15 bytes per spill »relative times of incoming muons –abnormal and 10% events (6 Tb) –60 bytes/event additionally –overall: ~ 20 Tb per 1 ppm measurement

30. Beamtime and Run Plans Year 1 –Build prototype SuperTriangles –Tube and Base selection –Establish funding for full detector –Use  SR setup to establish target depolarization properties 1 week plus collaboration with experts –Tests of 2 SuperTriangles system with modest DC surface  beam (no chopper, low intensity) light output asymmetry cross talk etc. 1 week plus setup of 1-2 weeks

31. Beamtime and Run Plans Year 2 –Build  Lan detector at home institutes –Build mechanical carriage –Build WFDs –Develop DAQ system and begin purchases or components –At PSI Test of half or more of full system to debug system issues Use DC beam (no chopper yet unless it is ready) Tests of detector uniformities Development of software energy/time algorithms for online CPUs Make a 10 ppm measurement of   4 weeks beam plus setup 2 weeks

32. Beamtime and Run Plans Year 3 –Calibration system finalization –Complete electronics –Complete DAQ –Complete chopper and beamline installation modifications –At PSI Test beamline and chopping –2 weeks of beamtime for tuning and establishing parameters Debug full system –1 week for tests and debugging Make a 1 ppm measurement of   with target #1 –6 weeks beam Year 4 (if necessary) Make a 1 ppm measurement of   with target #2 –6 weeks beam + 2 weeks setup again

33. CONCLUSION A new measurement of the muon lifetime (and hence G F ) is necessary to reap the full benefit of precision measurements at present and future accelerators and recent theoretical progress. A chopped beam time-structure available at PSI should make it possible to improve the measurement of G F by a factor of 10-20, in a modest amount of time. Our collaboration is capable of carrying out this task. While questions remain, we believe the basic experimental concept is sound. It is also complementary to other proposed approaches. Our basic request to PSI is to help to establish the beam and chopping device. –The MORE scheme looks appropriate with modest changes –We are very hopeful to have enticed local experts to collaborate!!