Material for speakers: Difference between revisions
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[https://journals.aps.org/prd/abstract/10.1103/PhysRevD.80.013002 Vincenzo Cirigliano, Ryuichiro Kitano, Yasuhiro Okada, and Paula Tuzon
Phys. Rev. D 80, 013002 (2009)]
PIP-II public web site
E. Pozdeyev, Rare Processes and Precision Frontier Town Hall (2020)
[3] "Early considerations for muon collider targetry at CERN"
COMET tracker (2020 NIM) [4]
COMET tracker (2016 slides) [5]
[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)
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<li> https://journals.aps.org/prd/abstract/10.1103/PhysRevD.80.013002 | <li> [https://journals.aps.org/prd/abstract/10.1103/PhysRevD.80.013002 Vincenzo Cirigliano, Ryuichiro Kitano, Yasuhiro Okada, and Paula Tuzon | ||
Phys. Rev. D 80, 013002 (2009)] | |||
=PIP-II accelerator= | =PIP-II accelerator= |
Revision as of 23:15, 16 July 2021
Mu2e
Mu2e public results and material for speakers
Theory
References
PIP-II accelerator
Beamline
Production target
Production solenoid
Tracking
References
Calorimeter
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.