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A few thoughts on eee Chih-Hsiang Cheng, Bertrand Echenard, David Hitlin, Frank Porter California Institute of Technology Intensity frontier workshop Argonne April 2013 Probing Lorentz structure of New Physics Y. Okada et al. , PRD 61


  1. A few thoughts on µ → eee Chih-Hsiang Cheng, Bertrand Echenard, David Hitlin, Frank Porter California Institute of Technology Intensity frontier workshop Argonne – April 2013

  2. Probing Lorentz structure of New Physics Y. Okada et al. , PRD 61 (200) 094001 Dalitz plot of µ → eee defined with help of the muon polarization carry information on chirality and Lorentz structure of CLFV couplings (same for τ → µµµ ) Generic Lagrangian Positron 1 vs Positron 2 (E 1 > E 2 ) x i = 2E i /m µ A R,L photon-penguin coupling, contributes to µ → e γ , µ → eee g i 4-point contact interaction, contributes to µ → eee Need at least dozens of events and a polarized muons Bertrand Echenard Intensity frontier Workshop - April 2013 p.2

  3. Probing Lorentz structure of New Physics B.M. Dassinger et al. , JHEP 0710 (2007) 039 Similar situation in τ → µµµ Need at least dozens of events and a polarized taus Bertrand Echenard Intensity frontier Workshop - April 2013 p.3

  4. Reference: the mu3e experiment arXiv:1301:6113 Reference: the mu3e design N. Berger N. Berger Achieve a µ → eee mass resolution ~ 520 keV Time resolution ~50 ps (tile) / ~500 ps (fiber) Bertrand Echenard Intensity frontier Workshop - April 2013 p.4

  5. Sensitivity of mu3e experiment N. Berger Accidental background not shown here, level similar to µ → eee νν in size but flat in mass Mu3e goal Need to beat down these backgrounds → better timing and mass resolution Bertrand Echenard Intensity frontier Workshop - April 2013 p.5

  6. Active target An active target could help by further constraining the decay vertex and improving the time resolution. This would reduce the accidentals (typically a few muon decay / ns in target) • improve mass resolution, thus reducing the µ → eee νν background • See D. Brown talk on active target Bertrand Echenard Intensity frontier Workshop - April 2013 p.6

  7. FastSim Chih-Hsiang Cheng Simulation of prototype detector for µ → e γ with FastSim Use the same tool to simulate a detector for µ → eee with an active target. see C.H. Cheng talk on µ → e γ Bertrand Echenard Intensity frontier Workshop - April 2013 p.7

  8. Outlook Plan to study a “mu3e-like” configuration with FastSim using an active target to see if we can • improve the mass resolution • Improve the accidentals rejection Explore alternative geometries Any good idea is welcome. Bertrand Echenard Intensity frontier Workshop - April 2013 p.8

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