MeasurementIntro: Difference between revisions

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==Overview of Theories that Mu2e Will Probe==
==Overview of Theories that Mu2e Will Probe==
Overview of models that will be tested and how they are motivated
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

A Brief History of the Measurement

Planned Future Experiments (Mu2e II)