Material for speakers: Difference between revisions
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[3] "Early considerations for muon collider targetry at CERN"
COMET tracker (2020 NIM) [4]
COMET tracker (2016 slides) [5]
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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> | <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> | ||
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=PIP-II accelerator= | =PIP-II accelerator= | ||
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<li style="display: inline-block; vertical-align: top;"> [[File:BallDeformation.png|thumb|top]] </li> | <li style="display: inline-block; vertical-align: top;"> [[File:BallDeformation.png|thumb|top]] </li> | ||
<li style="display: inline-block; vertical-align: top;"> [[File:HRScaptioned.png|thumb|top]] </li> | <li style="display: inline-block; vertical-align: top;"> [[File:HRScaptioned.png|thumb|top]] </li> | ||
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==References== | ==References== | ||
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<li style="display: inline-block; vertical-align: top;"> [[File:AmbroseCPAD Mu2e Tracker 19.png|thumb|top]] </li> | <li style="display: inline-block; vertical-align: top;"> [[File:AmbroseCPAD Mu2e Tracker 19.png|thumb|top]] </li> | ||
<li style="display: inline-block; vertical-align: top;"> [[File:AmbroseCPAD Mu2e Tracker 20.png|thumb|top]] </li> | <li style="display: inline-block; vertical-align: top;"> [[File:AmbroseCPAD Mu2e Tracker 20.png|thumb|top]] </li> | ||
</ul> | |||
==References== | ==References== | ||
Revision as of 18:59, 16 July 2021
Mu2e
Mu2e public results and material for speakers
Theory
-
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].
PIP-II accelerator
Beamline
Production target
References
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.
References
Calorimeter
- [6] "A Novel Scintillator Detector for the Mu2e-II Experiment and a Muon Tomography Probe of the Interior of the Great Pyramid"
- [7] Muon-ion collider for BNL (2021)
- [8] Mu2e-II Snowmass 22 Letter of Interest (2020)
- [9] 1st muon community meeting (CERN), 20-21 May 2020
- [10] Mu2e-II theory Snowmass 22 Letter of Interest (2020)
- [11] COMET Phase-I TDR (2020)
- [12] Muon colliders (2019)
- [13] Mu2e-II Expression of Interest (2018)
