Mu2e and Project X, September 3, 2008 E Prebys Background: Proton Economics in Project X Era* Assume  9mA*1ms = 5.3x10 13 protons/linac “blast”  Main.

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Presentation transcript:

Mu2e and Project X, September 3, 2008 E Prebys Background: Proton Economics in Project X Era* Assume  9mA*1ms = 5.3x10 13 protons/linac “blast”  Main Injector ramp time + = 1 *Prebys and Ankenbrandt, ProdDev-DOC R. Zwaska, FNAL-BEAMDOC-2393 NOT simply linear! Assuming no stretcher ring

Mu2e and Project X, September 3, 2008 E Prebys Power and Protons 2

Mu2e and Project X, September 3, 2008 E Prebys 3 Muon-to-Electron Conversion:  +N  e+N Similar to  e  with important advantages:  No combinatorial background  Because the virtual particle can be a photon or heavy neutral boson, this reaction is sensitive to a broader range of BSM physics Relative rate of  e  and  N  eN  is the most important clue regarding the details of the physics  105 MeV e - When captured by a nucleus, a muon will have an enhanced probability of exchanging a virtual particle with the nucleus. This reaction recoils against the entire nucleus, producing the striking signature of a mono-energetic electron carrying most of the muon rest energy

Mu2e and Project X, September 3, 2008 E Prebys 4 Previous muon decay/conversion limits (90% C.L.) Rate limited by need to veto prompt backgrounds!  >e Conversion: Sindrum II LFV  Decay: High energy tail of coherent Decay-in-orbit (DIO)

Mu2e and Project X, September 3, 2008 E Prebys 5 Mu2e (MECO) Philosophy Eliminate prompt beam backgrounds by using a primary beam with short proton pulses with separation on the order of a muon life time Design a transport channel to optimize the transport of right-sign, low momentum muons from the production target to the muon capture target. Design a detector to strongly suppress electrons from ordinary muon decays ~100 ns ~1-2  s Prompt backgrounds live window

Mu2e and Project X, September 3, 2008 E Prebys 6 Beam Related Rates Cut ~700 ns after pulse to eliminate most serious prompt backgrounds.

Mu2e and Project X, September 3, 2008 E Prebys Beam Needs Bunch spacing  Veto window: 700 ns  Captured lifetime: 880 ns (Al target)  Average arrival time: 300 ns relative to first Rate:  Limited by straw chambers  ~8x10 13 p/sec 7 ns ~1.7  sec

Mu2e and Project X, September 3, 2008 E Prebys Modes of running project X Assume slow extraction by “blast”  1 “blast” = 9mA*1ms = 5.6e13 (protons)/(1.4 s cycle)  = 4e13 p/s on average (!!)  = 50 kW average beam power  = 8e20/yr (2e7 seconds) Compare to baseline proposal  6*4e12 protons/(1.33 s NOvA cycle) = 1.8e13 p/s on average  = 23 kW average beam power = 3.6e20 Modes of operation considered  All “extra” blasts, extracted one at a time 1 blast in 200 ms (sharing) = 14% duty factor 4 in 800 ms = 57% duty factor 2 blasts in 800 ms (timeline hog) = 57% duty factor, 50% “usage factor” 1 blast in 800 ms (super hog) = 57% duty factor, 25% usage factor 4/23/08

Mu2e and Project X, September 3, 2008 E Prebys Rates under various scenarios Rate limit comes from straw chamber singles rate Assume we cannot push it much higher than the MECO proposal (500 kHz during live window)  Assume factor of ~2 9 ModeDuty FactorPeak RateAverage Rate protons/skWrel to MECORel. w/stretchkWp/yearrel. to MECO MECO50%4.0E E Phase 1100%1.8E E in 200ms14%2.8E E in 800ms57%2.8E E in 800ms57%1.4E E in 800ms57%7.0E E

Mu2e and Project X, September 3, 2008 E Prebys Conclusion If we extract beam directly from the Recycler, then only the “super hog” mode appears to obviously benefit Mu2e  Double the protons/yr rel. to phase 1 With a beam stretcher (assuming we get all of it), we could take an additional blast  Quadruple rate/yr rel. to phase 1 10

Mu2e and Project X, September 3, 2008 E Prebys BACKUP SLIDES 11

Mu2e and Project X, September 3, 2008 E Prebys  e Conversion vs.  e  12 Courtesy: A. de Gouvea ? ? ? Sindrum II MEGA MEG proposal We can parameterize the relative strength of the dipole and four fermi interactions. This is useful for comparing relative rates for  N  eN and  e 