A. La Rosa
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View article: Physics Informed Neural Networks for design optimisation of diamond particle detectors for charged particle fast-tracking at high luminosity hadron colliders
Physics Informed Neural Networks for design optimisation of diamond particle detectors for charged particle fast-tracking at high luminosity hadron colliders Open
Future high-luminosity hadron colliders demand tracking detectors with extreme radiation tolerance, high spatial precision, and sub-nanosecond timing. 3D diamond pixel sensors offer these capabilities due to diamond's radiation hardness an…
View article: Hybrids pre-production results for the CMS Outer Tracker Phase-2 Upgrade
Hybrids pre-production results for the CMS Outer Tracker Phase-2 Upgrade Open
The CMS Tracker Phase-2 Upgrade requires the production of two co-planar strip sensor (2S) modules, and strip and macro-pixel sensor (PS) modules to cope with the requirements of the HL-LHC. Altogether 47520 hybrid circuits are required to…
View article: Weighted CTDI Equation for 3D Rotational Angiography: A Monte Carlo Study
Weighted CTDI Equation for 3D Rotational Angiography: A Monte Carlo Study Open
This study aims to verify the weighted Computed Tomography Dose Index (CTDIw) coefficients of 3D rotational angiography (3DRA) procedure using Monte Carlo simulation. The Monte Carlo simulation EGSnrc usercode was employed for 3D dose simu…
View article: Hybrid designs and kick-off batch production experience for the CMS Phase-2 Upgrade
Hybrid designs and kick-off batch production experience for the CMS Phase-2 Upgrade Open
The CMS Tracker Phase-2 Upgrade requires the production of new sensor modules to cope with the requirements of the HL-LHC. The two main building blocks of the Outer Tracker are the Strip-Strip and Pixel-Strip modules. All-together 47'520 h…
View article: Gain layer degradation study after neutron and proton irradiations in Low Gain Avalanche Diodes
Gain layer degradation study after neutron and proton irradiations in Low Gain Avalanche Diodes Open
The high-luminosity upgrade of the ATLAS and CMS experiments includes dedicated sub-detectors to perform the time-stamping of minimum ionizing particles (MIPs). These detectors will be exposed up to fluences in the range of 1.5-2.5 × 10 15…
View article: Gain layer degradation study after neutron and proton irradiations in Low Gain Avalanche Diodes
Gain layer degradation study after neutron and proton irradiations in Low Gain Avalanche Diodes Open
The high-luminosity upgrade of the ATLAS and CMS experiments includes dedicated sub-detectors to perform the time-stamping of minimum ionizing particles (MIPs). These detectors will be exposed up to fluences in the range of 1.5 - 2.5e15 ne…
View article: Quality Inspection Aspects of Hybrid Prototypes for the CMS Outer Tracker Upgrade at HL-LHC
Quality Inspection Aspects of Hybrid Prototypes for the CMS Outer Tracker Upgrade at HL-LHC Open
At the High Luminosity LHC (HL-LHC), the CMS experiment will need to operate at up to 200 interactions per 25 ns beam crossing time and with up to 4000 fb −1 of integrated luminosity. To achieve the physics goals the experiment needs to im…
View article: The Upgrade of the CMS Tracker at HL-LHC
The Upgrade of the CMS Tracker at HL-LHC Open
In the high luminosity scenario of the LHC (HL-LHC), which will bring the instantaneous luminosity up to 7.5\\,$\\times$\\,$10^{34}$\\,cm$^{-2}$s$^{-1}$, ATLAS and CMS will need to operate at up to 200 interactions per 25\\,ns beam crossin…
View article: Prototyping of Hybrid Circuits for the CMS Phase-2 Outer Tracker Upgrade at the HL-LHC
Prototyping of Hybrid Circuits for the CMS Phase-2 Outer Tracker Upgrade at the HL-LHC Open
High Density Interconnect hybrids are being developed for the CMS tracker Phase-2 upgrade for the HL-LHC. These hybrids are flexible circuits laminated to carbon fiber composite stiffeners and are assembled with flip-chips, passives and co…
View article: The CMS Outer Tracker for the High Luminosity LHC upgrade
The CMS Outer Tracker for the High Luminosity LHC upgrade Open
The High Luminosity Large Hadron Collider (HL-LHC) at CERN is expected to collide protons at a centre-of-mass energy of 14 TeV and to reach the unprecedented peak instantaneous luminosity of 5–7.5 × 1034 cm−2 s−1 with an average number of …
View article: TCAD simulations of pixel sensors for the ATLAS ITk upgrade and performance of annealed planar pixel modules
TCAD simulations of pixel sensors for the ATLAS ITk upgrade and performance of annealed planar pixel modules Open
For the high luminosity phase of the Large Hadron Collider to start operation around 2026, a major upgrade of the ATLAS Inner Tracker (ITk) is in preparation. Thanks to their low power dissipation and high charge-collection efficiency afte…
View article: Performance of irradiated thin n-in-p planar pixel sensors for the ATLAS Inner Tracker upgrade
Performance of irradiated thin n-in-p planar pixel sensors for the ATLAS Inner Tracker upgrade Open
The ATLAS collaboration will replace its tracking detector with new all\nsilicon pixel and strip systems. This will allow to cope with the higher\nradiation and occupancy levels expected after the 5-fold increase in the\nluminosity of the …
View article: The ATLAS Insertable B-Layer: from construction to operation
The ATLAS Insertable B-Layer: from construction to operation Open
The ATLAS Insertable B-Layer (IBL) is the innermost layer of pixel detectors, and was installed in May 2014 at a radius of 3.3 cm from the beam axis, between the existing Pixel detector and a new smaller radius beam-pipe. The new detector,…
View article: Characterization of Novel Thin N-in-P Planar Pixel Modules for the ATLAS Inner Tracker Upgrade
Characterization of Novel Thin N-in-P Planar Pixel Modules for the ATLAS Inner Tracker Upgrade Open
The ATLAS experiment will undergo a major upgrade of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) to start operation in 2026. The most severe challenges are to be faced by the innermost layers of the pixel de…
View article: The ATLAS Insertable B-Layer: from construction to operation
The ATLAS Insertable B-Layer: from construction to operation Open
The ATLAS Insertable B-Layer (IBL) is the innermost layer of pixel detectors, and was installed in May 2014 at a radius of 3.3 cm from the beam axis, between the existing Pixel detector and a new smaller radius beam-pipe. The new detector,…
View article: Characterization of novel thin N-in-P planar pixel modules for the ATLAS inner tracker upgrade
Characterization of novel thin N-in-P planar pixel modules for the ATLAS inner tracker upgrade Open
The ATLAS experiment will undergo a major upgrade of the tracker system in view of the high luminosity phase of the LHC (HL-LHC) to start operation in 2026. The most severe challenges are to be faced by the innermost layers of the pixel de…
View article: Irradiation induced effects in the FE-I4 front-end chip of the ATLAS IBL detector
Irradiation induced effects in the FE-I4 front-end chip of the ATLAS IBL detector Open
The ATLAS Insertable B-Layer (IBL) detector was installed into the ATLAS experiment in 2014 and has been in operation since 2015. During the first year of IBL data taking an increase of the low voltage currents associated with the FE-I4 fr…
View article: Measurement of fiducial differential cross sections of gluon-fusion production of Higgs bosons decaying to $WW^*\\rightarrow\\textit{e}\\nu\\mu\\nu$ with the ATLAS detector at $\\sqrt{s}=8$ TeV
Measurement of fiducial differential cross sections of gluon-fusion production of Higgs bosons decaying to $WW^*\\rightarrow\\textit{e}\\nu\\mu\\nu$ with the ATLAS detector at $\\sqrt{s}=8$ TeV Open
This paper describes a measurement of fiducial and differential cross sections of gluon-fusion Higgs boson production in the $H\\rightarrow WW^*\\rightarrow \\textit{e}\\nu\\mu\\nu$ channel, using 20.3 fb$^{-1}$ of proton-proton collision …