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The analysis of a combined data set, totaling 3.6 × 10(14) stopped muons on target, in the search for the lepton flavor violating decay μ(+) → e(+)γ is presented. The data collected by the MEG experiment at the Paul Scherrer Institut show no excess of events compared to background expectations and yield a new upper limit on the branching ratio of this decay of 5.7 × 10(-13) (90% confidence level). This represents a four times more stringent limit than the previous world best limit set by MEG.

The MEG experiment, designed to search for the µ + → e + γ decay at a 10 −13 sensitivity level, completed datataking in 2013. In order to increase the sensitivity reach of the experiment by an order of magnitude to the level of 6 × 10 −14 for the branching ratio, a total upgrade, involving substantial changes to the experiment, has been undertaken, known as MEG II. We present both the motivation for the upgrade and a detailed overview of the design of the experiment and of the expected detector performance.

Neural precursor cells (NPCs) in the mouse neocortex generate various neuronal and glial cell types in a developmental stage–dependent manner. Most NPCs lose their neurogenic potential during development, although the underlying mechanisms of this process are not fully understood. We found that the chromatin of mouse NPCs gradually becomes more condensed and less dynamic on a global scale during neocortical development. Furthermore, we found high mobility group A (HMGA) proteins to be essential for the open chromatin state of NPCs at early developmental stages. Knockdown of HMGA proteins in early-stage NPCs reduced their neurogenic potential. Conversely, overexpression of HMGA proteins conferred neurogenic potential on late-stage NPCs, an effect that was antagonized by coexpression of a histone H1 mutant that inhibits chromatin opening. Thus, HMGA proteins contribute to the neurogenic potential of NPCs in the early stages of neocortical development, possibly through induction of an open chromatin state.

The Tokai-to-Kamioka (T2K) experiment studies neutrino oscillations using an off-axis muon neutrino beam with a peak energy of about 0.6 GeV that originates at the J-PARC accelerator facility. Interactions of the neutrinos are observed at near detectors placed at 280 m from the production target and at the far detector -Super-Kamiokande (SK) -located 295 km away. The flux prediction is an essential part of the successful prediction of neutrino interaction rates at the T2K detectors and is an important input to T2K neutrino oscillation and cross section measurements. A FLUKA and GEANT3 based simulation models the physical processes involved in the neutrino 3 production, from the interaction of primary beam protons in the T2K target, to the decay of hadrons and muons that produce neutrinos. The simulation uses proton beam monitor measurements as inputs. The modeling of hadronic interactions is re-weighted using thin target hadron production data, including recent charged pion and kaon measurements from the NA61/SHINE experiment. For the first T2K analyses the uncertainties on the flux prediction are evaluated to be below 15% near the flux peak. The uncertainty on the ratio of the flux predictions at the far and near detectors is less than 2% near the flux peak.