Material for speakers

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].
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  Tail of the electron spectrum for DIOs and for two [math]\displaystyle{ \mu\to eX }[/math] scenarios [2].

PIP-II accelerator

PIP-II public web site

Beamline

Production target

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References

[3] "Early considerations for muon collider targetry at CERN"

Production solenoid

Tracking

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  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.
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References

COMET tracker (2020 NIM) [4]

COMET tracker (2016 slides) [5]

Calorimeter

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

The Mu2e-II Cosmic Ray Veto will need to cope with roughly a factor 3 higher instantaneous rates from accelerator compared with Mu2e as well as a factor of three higher live time (i.e., cosmic rays), because of the higher duty factor for Mu2e-II compared with Mu2e.

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References

[6] "A Novel Scintillator Detector for the Mu2e-II Experiment and a Muon Tomography Probe of the Interior of the Great Pyramid"

Sensitivity

References

[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)