3,242 research outputs found
First experimental results of the spatial resolution of RSD pad arrays read out with a 16-ch board
Resistive Silicon Detectors (RSD, also known as AC-LGAD) are innovative silicon sensors, based on the LGAD technology, characterized by a continuous gain layer that spreads across the whole sensor active area. RSDs are very promising tracking detectors, thanks to the combination of the built-in signal sharing with the internal charge multiplication, which allows large signals to be seen over multiple read-out channels. This work presents the first experimental results obtained from a 34 array with 200~\mum~pitch, coming from the RSD2 production manufactured by FBK, read out with a 16-ch digitizer. A machine learning model has been trained, with experimental data taken with a precise TCT laser setup, and then used to predict the laser shot positions, finding a spatial resolution of ~ 5.5 um
Probing effective field theory operators in the associated production of top quarks with a Z boson in multilepton final states at √s = 13 TeV
Measurement of the top quark mass using events with a single reconstructed top quark in pp collisions at √s = 13 TeV
Combined searches for the production of supersymmetric top quark partners in proton–proton collisions at √s=13Te
Search for a heavy Higgs boson decaying into two lighter Higgs bosons in the ττbb final state at 13 TeV
Measurement of the Z boson differential production cross section using its invisible decay mode (Z → νν¯) in proton-proton collisions at √s = 13 TeV
The second production of RSD (AC-LGAD) at FBK
In this contribution we describe the second run of RSD (Resistive AC-Coupled
Silicon Detectors) designed at INFN Torino and produced by Fondazione Bruno
Kessler (FBK), Trento. RSD are n-in-p detectors intended for 4D particle
tracking based on the LGAD technology that get rid of any segmentation implant
in order to achieve the 100% fill-factor. They are characterized by three
key-elements, (i) a continuous gain implant, (ii) a resistive n-cathode and
(iii) a dielectric coupling layer deposited on top, guaranteeing a good spatial
reconstruction of the hit position while benefiting from the good timing
properties of LGADs. We will start from the very promising results of our RSD1
batch in terms of tracking performances and then we will move to the
description of the design of the RSD2 run. In particular, the principles
driving the sensor design and the specific AC-electrode layout adopted to
optimize the signal confinement will be addressed
- …
