133 citations · 318 across the 12 of their papers we have counts for
6 papers · 1 filter
Characterization of the first full-size production for ePIC TOF layers
M. Davis, G. Stage, A. Borjigin +13
Low-Gain Avalanche Detectors (LGADs) are characterized by a fast rise time (500 ps) and extremely good time resolution (down to 17 ps). The intrinsic low granularity of LGADs and t…
Optimization of the Gain Layer Design of Ultra-Fast Silicon Detectors
Federico Siviero, Roberta Arcidiacono, Giacomo Borghi +17
In the past few years, the need of measuring accurately the spatial and temporal coordinates of the particles generated in high-energy physics experiments has spurred a strong R\&D…
Comparison of 35 and 50 μm thin HPK UFSD after neutron irradiation up to 6*10^15 neq/cm^2
Y. Zhao, N. Cartiglia, E. Estrada +13
We report results from the testing of 35 μm thick Ultra-Fast Silicon Detectors (UFSD produced by Hamamatsu Photonics (HPK), Japan and the comparison of these new results to data re…
Radiation resistant LGAD design
M. Ferrero, R. Arcidiacono, M. Barozzi +16
In this paper, we report on the radiation resistance of 50-micron thick LGAD detectors manufactured at the Fondazione Bruno Kessler employing several different doping combinations…
Radiation Hardness of Thin Low Gain Avalanche Detectors
G. Kramberger, M. Carulla, E. Cavallaro +18
Low Gain Avalanche Detectors (LGAD) are based on a n++-p+-p-p++ structure where an appropriate doping of the multiplication layer (p+) leads to high enough electric fields for impa…
Properties of HPK UFSD after neutron irradiation up to 6e15 n/cm2
Z. Galloway, V. Fadeyev, P. Freeman +27
In this paper we report results from a neutron irradiation campaign of Ultra-Fast Silicon Detectors (UFSD) with fluences of 1e14, 3e14, 6e14, 1e15, 3e15, 6e15 n/cm2. The UFSD used…