Material for speakers: Difference between revisions
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<li style="display: inline-block; vertical-align: top;"> [[File:Zscenarios.png|thumb|top|Z dependence of µ → e conversion rates for some | <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> | sample scenarios [https://www.snowmass21.org/docs/files/summaries/RF/SNOWMASS21-RF5_RF0-TF6_TF0_Heeck-043.pdf].]] </li> | ||
<li style="display: inline-block; vertical-align: top;"> [[File:Mu2eXspectrum.png|thumb|top|Tail of the electron spectrum for DIOs and for two <math>\mu\to eX</math> 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 22:56, 18 June 2021
Mu2e
Mu2e public results and material for speakers
Theory
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Z dependence of µ → e conversion rates for some sample scenarios [1]. -
Tail of the electron spectrum for DIOs and for two [math]\displaystyle{ \mu\to eX }[/math] scenarios [2]. -
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.
