Introduction to the MEG/MEG II experiment

The MEG/MEG II experiments at Paul Scherrer Institut (PSI) have been designed to search for the charged-lepton-flavour-violating rare muon decay, μ+ → e+γ, with a sensitivity of 10-13–10-14.
The decay μ+ → e+γ is strongly suppressed down to 10-54 by the Standard Model with neutrino oscillation, but is predicted to have a sizable branching ratio of 10-11–10-14 by various new physics models beyond the Standard Model. Thus, μ+ → e+γ is an interesting probe to search for new physics.
We utilise the most intense DC muon beam at PSI at 107 μ/s and have developed innovative detectors to precisely measure decay products of positrons and photons. Using them, we have been updating the most stringent upper limit on the branching ratio of μ+ → e+γ and leading experiments to search for charged lepton flavour violation (CLFV) with muons, as shown below.
CLFV searches with muons
History of experimental searches for CLFV with muons. Solid markers correspond to our publications, and a solid star is our latest results.
We plan to continue to collect data until 2026, searching for μ+ → e+γ with an approximate sensitivity of 6 × 10-14.
Other physics have been investigated with the MEG/MEG II apparatus.
We have precisely measured the branching ratio of a radiative muon decay in the Standard Model, μ+ → e+ννγ. Searches for new particles, such as axion-like particle, have also been performed in charged-lepton-flavour-violating channels of μ+ → e+aγ and μ+ → e+X, X → γγ. Moreover, we have been searching for a hypothetical X17 particle, reported by the ATOMKI collaboration.
Our physics results are listed on the Documents page.

K. Yamamoto, 9th May 2025