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Projected sensitivity to light WIMP-like particles of the BULLKID-DM experiment
Matteo Folcarelli, A. Acevedo-Rentería, L. E. Ardila-Perez +39
BULLKID-DM is an experiment designed for the direct searches of particle dark matter candidates with mass around 1 GeV, or below, and cross-section with nucleons smaller than $10^{…
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…
Real-Time Readout System Design for the BULLKID-DM Experiment: Enhancing Dark Matter Search Capabilities
T. Muscheid, R. Gartmann, L. E. Ardila-Perez +41
The BULLKID-DM experiment aims to detect WIMP-like potential Dark Matter particles with masses below 1 GeV/c^2. Sensing these particles is challenging, as it requires nuclear recoi…
Energy calibration of bulk events in the BULLKID detector
M. Folcarelli, D. Delicato, A. Acevedo-Rentería +39
BULLKID is a cryogenic, solid-state detector designed for direct searches of particle Dark Matter candidates, with mass GeV/c, and coherent neutrino-nucleus scatte…
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…