In May 2016 the MEG experiment published the world's leading upper limit on the branching ratio of this decay:
at 90% confidence level, 2 based on data collected in 2009–2013. This improved the MEG limit from the prior MEGA experiment3 by a factor of about 28.
MEG uses a continuous muon beam (3 × 107/s) incident on a plastic target. The decay is reconstructed to look for a back-to-back positron and monochromatic photon (52.8 MeV). A liquid xenon scintillator with photomultiplier tubes measure the photon energy, and a drift chamber in a magnetic field detects the positrons.
The MEG collaboration presented upgrade plans for MEG-II at the Particles and Nuclei International Conference 2014, with one order of magnitude greater sensitivity, and increased muon production, to begin data taking in 2017.4 More experiments are planned to explore rare muon transitions, such as Comet (experiment), Mu2e and Mu3e.
"MEG goes in search of the forbidden". CERN Courier. 27 July 2004. http://cerncourier.com/cws/article/cern/29118 ↩
Baldini, A. M.; et al. (MEG collaboration) (May 2016). "Search for the Lepton Flavour Violating Decay μ+→e+γ with the Full Dataset of the MEG Experiment". arXiv:1605.05081 [hep-ex]. /wiki/ArXiv_(identifier) ↩
Brooks, M. L.; et al. (MEGA Collaboration) (23 August 1999). "New limit for the lepton-family-number nonconserving decay μ+→e+γ". Physical Review Letters. 83 (8): 1521–1524. arXiv:hep-ex/9905013. Bibcode:1999PhRvL..83.1521B. doi:10.1103/PhysRevLett.83.1521. S2CID 119354296. https://zenodo.org/record/1233921 ↩
Renga, F (2014). "Latest results of MEG and status of MEG-II". arXiv:1410.4705 [hep-ex]. /wiki/ArXiv_(identifier) ↩