Material for speakers: Difference between revisions

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=Theory=
=Theory=
<div><ul>
<li style="display: inline-block; vertical-align: top;"> [[File:Zscenarios.png|thumb|top|Z dependence of µ → e conversion rates for some
sample scenarios [https://www.snowmass21.org/docs/files/summaries/RF/SNOWMASS21-RF5_RF0-TF6_TF0_Heeck-043.pdf].]] </li>


=PIP-II accelerator=
=PIP-II accelerator=

Revision as of 22:49, 18 June 2021

Mu2e

Mu2e public results and material for speakers

Theory

  • Z dependence of µ → e conversion rates for some sample scenarios [1].
  • PIP-II accelerator

    PIP-II public web site

    Beamline

    Production target

    • ProductionTargetRotatingRodsWcaption-IPAC214MP.png
    • ProductionTargetDesignsFixedGranular4MP-IPAC21.png
    • ProductionTargetDesignsConveyor4MP-IPAC21.png
    • ComparisonTable4MP-IPAC21.png
    • BallDeformation.png
    • HRScaptioned.png
    • Production solenoid

      Tracking

      • Slide illustrating the requirement on track resolution for Mu2e-II compared with Mu2e. Noe that the resolution has contributions from several sources. The blue dashed curve on each plot indicates the electron spectrum from muon decays in orbit (DIOs). The red curves show the conversion electron spectrum for the values of [math]\displaystyle{ R_{\mu e} }[/math] indicated in the legends.
      • AmbroseCPAD Mu2e Tracker 184MP.jpg
      • AmbroseCPAD Mu2e Tracker 19.png
      • AmbroseCPAD Mu2e Tracker 20.png
      • Calorimeter

        • Effect of yttrium doping on suppressing the slow component in BaF[math]\displaystyle{ _2 }[/math]
        • Cosmic Ray Veto

          Sensitivity

          References

        • [2] Mu2e-II Snowmass 22 Letter of Interest (2020)
        • [3] Mu2e-II theory Snowmass 22 Letter of Interest (2020)
        • [4] Mu2e-II Expression of Interest (2018)