MeasurementIntro: Difference between revisions
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==Overview of Theories that Mu2e Will Probe== | ==Overview of Theories that Mu2e Will Probe== | ||
MSSM with right handed neutrinos | |||
SUSY with R-parity Violations | |||
Leptoquarks | |||
New Gauge Bosons | |||
Large Extra Dimensions | |||
Non-Minimal Higgs Structure | |||
==A Brief History of the Measurement== | ==A Brief History of the Measurement== | ||
==Planned Future Experiments (Mu2e II)== | ==Planned Future Experiments (Mu2e II)== |
Revision as of 18:45, 8 February 2018
Introduction to the Measurement
The Mu2e Experiment will measure the rate of muons that convert directly into electrons in the field of a nucleus without the accompanying neutrinos that the standard model of particle physics predicts. This process is all but forbidden in the standard model due to the apparent conservation of a property known as “flavor”. Muons have one flavor and electrons another. This means if flavor is conserved, a muon cannot decay to electrons without carrying forward the muon flavor in the interaction with the production of a muon neutrino. Likewise, an electron cannot appear in the decay without the cancellation of this new flavor with an anti-electron neutrino. Mu2e relies on momentum and energy conservation to determine whether the muon decay proceeded in a way that conserves flavor, or violates flavor conservation.
The Technique
(capture and monoenergetic signature)
Overview of Theories that Mu2e Will Probe
MSSM with right handed neutrinos
SUSY with R-parity Violations
Leptoquarks
New Gauge Bosons
Large Extra Dimensions
Non-Minimal Higgs Structure