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The Use of O2 in Gas Mixtures for Drift Chambers
A. M. Baldini, L. Bianco, H. Benmansour +20
The use of Oxygen in gas mixtures for drift chambers is highly discouraged because Oxygen, being strongly electronegative, is generally believed to lead, even in very small quantit…
Performances of a new generation tracking detector: the MEG II cylindrical drfit chamber
A. M. Baldini, H. Benmansour, G. Boca +28
The cylindrical drift chamber is the most innovative part of the MEG~II detector, the upgraded version of the MEG experiment. The MEG~II chamber differs from the MEG one because it…
Operation and performance of MEG II detector
MEG II Collaboration, K. Afanaciev, A. M. Baldini +82
The MEG II experiment, located at the Paul Scherrer Institut (PSI) in Switzerland, is the successor to the MEG experiment, which completed data taking in 2013. MEG II started fully…
The measuring systems of the wire tension for the MEG II Drift Chamber by means of the resonant frequency technique
A. M. Baldini, H. Benmansour, G. Cavoto +24
The ultra-low mass cylindrical drift chamber designed for the MEG II experiment is a challenging apparatus made of 1728 phi = 20 micron gold plated tungsten sense wires, 7680 phi =…
Detailed analysis of chemical corrosion of ultra-thin wires used in drift chamber detectors
A. M. Baldini, G. Cavoto, F. Cei +24
Ultra-thin metallic anodic and cathodic wires are frequently employed in low-mass gaseous detectors for precision experiments, where the amount of material crossed by charged parti…
The Drift Chamber of the MEG II experiment
G. F. Tassielli, A. M. Baldini, G. Cavoto +19
The MEG experiment at the Paul Scherrer Institut searches for the charged-Lepton-Flavor-Violating mu+ -> e+ gamma decay. MEG has already set the world best upper limit on the branc…