Fabrizio Aloschi
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Fabrizio Aloschi has a total of 375 co-authors. Here are the top co-authors by number of shared publications:
- Andrea Miano
Sezione INFN di Napoli
8 shared publications - A. Fiorillo
Sezione INFN di Napoli
7 shared publications - Adele Lauria
Sezione INFN di Napoli
7 shared publications - Albert De Roeck
CERN
7 shared publications - Alberto Blanco
Laboratory of Instrumentation and Experimental Particle Physics (LIP)
7 shared publications - Alexey Boyarsky
University of Leiden
7 shared publications
Latest Publications
- Open Access
- 26 October 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (10) , 1231
Measurement of di-muons from 400 GeV/c protons interacting in a thick molybdenum/tungsten target
Di-muon events emanating from a replica of the SHiP target at the CERN SPS (with a 400 GeV/c proton beam) contain a clear signal of $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}}$$ production. The target consisted of 13 interaction lengths of molybdenum and tungsten, followed by a 2.4m iron hadron absorber. The di-muon rate is in reasonable agreement with Monte Carlo simulation based on Pythia v8. However, the $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}} $$ rate observed in the data is much lower than predicted by the Monte Carlo simulation, which is advantageous for SHiP since muons with a large $$p_\textrm{T} $$ are more difficult to deflect by the active muon shield. For the center of mass rapidity ( $$y_{\textrm{cm}} $$ ) interval with the largest overlap with the NA50 measurement, $$0.3< y_{\textrm{cm}} < 0.6$$ , we obtain the production cross-section per nucleon $$\sigma ({J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}})/A$$ including the branching ratios of $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}} $$ decays into muons, $$B_{\mu ^+\mu ^-}$$ : $$B_{\mu ^+\mu ^-}\sigma ({J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}})/A=(1.18~\pm ~0.04~\pm ~0.10)~\textrm{nb}$$ /nucleon. This is to be compared to the NA50 extrapolated result (using a much thinner target): $$B_{\mu ^+\mu ^-}\sigma ({J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}})/A=(0.99~\pm ~0.04)~\textrm{nb}$$ /nucleon. Within the systematic errors, no significant enhancement due to secondary production of $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}}$$ inside the target is observed. An upper limit at 90% confidence level of possible contributions from secondary collisions of $$<32\%$$ is obtained.- 26 October 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (10) , 1231
Open AccessMeasurement of di-muons from 400 GeV/c protons interacting in a thick molybdenum/tungsten target
Di-muon events emanating from a replica of the SHiP target at the CERN SPS (with a 400 GeV/c proton beam) contain a clear signal of $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}}$$ production. The target consisted of 13 interaction lengths of molybdenum and tungsten, followed by a 2.4m iron hadron absorber. The di-muon rate is in reasonable agreement with Monte Carlo simulation based on Pythia v8. However, the $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}} $$ rate observed in the data is much lower than predicted by the Monte Carlo simulation, which is advantageous for SHiP since muons with a large $$p_\textrm{T} $$ are more difficult to deflect by the active muon shield. For the center of mass rapidity ( $$y_{\textrm{cm}} $$ ) interval with the largest overlap with the NA50 measurement, $$0.3< y_{\textrm{cm}} < 0.6$$ , we obtain the production cross-section per nucleon $$\sigma ({J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}})/A$$ including the branching ratios of $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}} $$ decays into muons, $$B_{\mu ^+\mu ^-}$$ : $$B_{\mu ^+\mu ^-}\sigma ({J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}})/A=(1.18~\pm ~0.04~\pm ~0.10)~\textrm{nb}$$ /nucleon. This is to be compared to the NA50 extrapolated result (using a much thinner target): $$B_{\mu ^+\mu ^-}\sigma ({J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}})/A=(0.99~\pm ~0.04)~\textrm{nb}$$ /nucleon. Within the systematic errors, no significant enhancement due to secondary production of $${J \hspace{-1.66656pt}/\hspace{-1.111pt}\psi \hspace{1.111pt}}$$ inside the target is observed. An upper limit at 90% confidence level of possible contributions from secondary collisions of $$<32\%$$ is obtained. - Open Access
- 1 September 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (9) , 1030
SND@LHC upgrade for the high-luminosity LHC: physics reach and installation scenarios
The SND@LHC experiment is currently taking data at the Large Hadron Collider (LHC), exploring the unique forward region at pseudorapidities $$7.2<\eta <8.4$$ . Its physics programme covers neutrinos originating from heavy-flavour decays and feebly interacting particles produced in proton–proton collisions. Building upon the successful operation of the present detector, this paper presents the physics reach of the approved SND@LHC upgrade for Run 4 of the LHC, and compares it with an alternative installation scenario. Lowering the detector by approximately 40 cm and shifting it horizontally by about 30 cm, while keeping it off-axis, increases the total neutrino interaction rate by a factor of five. The paper describes the design of the upgraded detector and compares the physics performance in both installation scenarios.- 1 September 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (9) , 1030
Open AccessSND@LHC upgrade for the high-luminosity LHC: physics reach and installation scenarios
The SND@LHC experiment is currently taking data at the Large Hadron Collider (LHC), exploring the unique forward region at pseudorapidities $$7.2<\eta <8.4$$ . Its physics programme covers neutrinos originating from heavy-flavour decays and feebly interacting particles produced in proton–proton collisions. Building upon the successful operation of the present detector, this paper presents the physics reach of the approved SND@LHC upgrade for Run 4 of the LHC, and compares it with an alternative installation scenario. Lowering the detector by approximately 40 cm and shifting it horizontally by about 30 cm, while keeping it off-axis, increases the total neutrino interaction rate by a factor of five. The paper describes the design of the upgraded detector and compares the physics performance in both installation scenarios. - Open Access
- 19 August 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (8) , 984
Measurement of the muon flux at SND@LHC
The SND@LHC experiment investigates neutrinos in the $$7.2< \eta < 8.4$$ forward pseudorapidity range. The detector consists of a veto system, a scintillating fiber tracker interleaved with emulsion cloud chambers, and a downstream muon system. Muons originating from collisions at ATLAS (IP1) constitute the primary background for CC neutrino interactions and determine the replacement frequency of the emulsion target. A precise characterization of this flux is therefore essential. In this work, we report the muon flux measured in the central $$31 \times 31$$ $$\textrm{cm}^2$$ fiducial area of the detector using data from 2023 through 2025. The measured fluxes for proton collisions are: (1.90±0.04) $$\times 10^{-2}$$ $$\text {nb/cm}^{2}$$ (2023), (3.76 ± 0.09) $$\times $$ $$\text {10}^{-2}$$ $$\text {nb/cm}^{2}$$ (2024), and (2.48 ± 0.05) $$\times 10^{-2}$$ $$\text {nb/cm}^{2}$$ (2025). A 2024 reference proton run at $$\sqrt{s} = 5.36\text { TeV}$$ yielded (4.21 ± 0.14) $$\times $$ $$\text {10}^{-2}$$ $$\text {nb/cm}^{2}$$ , providing a direct baseline for the heavy-ion energy regime. The measured fluxes for heavy-ion collisions are (3.11±0.12) $$\times \text {10}^{4}$$ $$\text {nb/cm}^{2}$$ , (5.53±0.22) $$\times 10^{4}$$ $$\text {nb/cm}^{2}$$ , and (3.24±0.13) $$\times \text {10}^{4}$$ $$\text {nb/cm}^{2}$$ in 2023, 2024, and 2025, respectively. Uncertainties are dominated by systematic effects, with the statistical component contributing $$\lesssim $$ 0.1% to the total uncertainty. These results are in agreement with Monte Carlo predictions.- 19 August 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (8) , 984
Open AccessMeasurement of the muon flux at SND@LHC
The SND@LHC experiment investigates neutrinos in the $$7.2< \eta < 8.4$$ forward pseudorapidity range. The detector consists of a veto system, a scintillating fiber tracker interleaved with emulsion cloud chambers, and a downstream muon system. Muons originating from collisions at ATLAS (IP1) constitute the primary background for CC neutrino interactions and determine the replacement frequency of the emulsion target. A precise characterization of this flux is therefore essential. In this work, we report the muon flux measured in the central $$31 \times 31$$ $$\textrm{cm}^2$$ fiducial area of the detector using data from 2023 through 2025. The measured fluxes for proton collisions are: (1.90±0.04) $$\times 10^{-2}$$ $$\text {nb/cm}^{2}$$ (2023), (3.76 ± 0.09) $$\times $$ $$\text {10}^{-2}$$ $$\text {nb/cm}^{2}$$ (2024), and (2.48 ± 0.05) $$\times 10^{-2}$$ $$\text {nb/cm}^{2}$$ (2025). A 2024 reference proton run at $$\sqrt{s} = 5.36\text { TeV}$$ yielded (4.21 ± 0.14) $$\times $$ $$\text {10}^{-2}$$ $$\text {nb/cm}^{2}$$ , providing a direct baseline for the heavy-ion energy regime. The measured fluxes for heavy-ion collisions are (3.11±0.12) $$\times \text {10}^{4}$$ $$\text {nb/cm}^{2}$$ , (5.53±0.22) $$\times 10^{4}$$ $$\text {nb/cm}^{2}$$ , and (3.24±0.13) $$\times \text {10}^{4}$$ $$\text {nb/cm}^{2}$$ in 2023, 2024, and 2025, respectively. Uncertainties are dominated by systematic effects, with the statistical component contributing $$\lesssim $$ 0.1% to the total uncertainty. These results are in agreement with Monte Carlo predictions. - Open Access
- 6 August 2026
- Published by Elsevier in International Journal of Disaster Risk Reduction
- Vol. 143
Integrating vulnerability and prioritization policies in post-earthquake recovery analysis of accessibility-based healthcare urban networks
- 6 August 2026
- Published by Elsevier in International Journal of Disaster Risk Reduction
- Vol. 143
Open AccessIntegrating vulnerability and prioritization policies in post-earthquake recovery analysis of accessibility-based healthcare urban networks
- Open Access
- 29 June 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (6)
Study of the Run-3 muon flux at the SND@LHC experiment
Long-range muons produced in proton–proton collisions at the ATLAS interaction point constitute the primary background for neutrino interaction searches at the SND@LHC experiment. This work presents a comprehensive characterization of the muon flux throughout LHC Run-3, benchmarking Monte Carlo simulations against experimental measurements. Measured and simulated muon rates agree within 10–15% across all Run-3 configurations. Following the substantial background increase in 2024 as a result of a beam optics change, the reversion to nominal optics in 2025 did not restore the 2022–2023 levels due to the unprecedented adoption of horizontal crossing in ATLAS. As indicated by simulation results, horizontal crossing enhanced the contribution of high-angle muons originating from diffractive proton losses in the LHC Dispersion Suppressor region. Their identification enabled the design of mitigation strategies that were experimentally validated. The simulation framework was also applied to the future high-luminosity LHC configuration, resulting in a considerable muon rate rise, driven by both the planned luminosity increase and the enlarged magnet aperture. Nevertheless, the upgrade from emulsion films to silicon vertex detectors will preserve the efficiency of the experiment even in such a high-rate environment.
- 29 June 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (6)
Open AccessStudy of the Run-3 muon flux at the SND@LHC experiment
Long-range muons produced in proton–proton collisions at the ATLAS interaction point constitute the primary background for neutrino interaction searches at the SND@LHC experiment. This work presents a comprehensive characterization of the muon flux throughout LHC Run-3, benchmarking Monte Carlo simulations against experimental measurements. Measured and simulated muon rates agree within 10–15% across all Run-3 configurations. Following the substantial background increase in 2024 as a result of a beam optics change, the reversion to nominal optics in 2025 did not restore the 2022–2023 levels due to the unprecedented adoption of horizontal crossing in ATLAS. As indicated by simulation results, horizontal crossing enhanced the contribution of high-angle muons originating from diffractive proton losses in the LHC Dispersion Suppressor region. Their identification enabled the design of mitigation strategies that were experimentally validated. The simulation framework was also applied to the future high-luminosity LHC configuration, resulting in a considerable muon rate rise, driven by both the planned luminosity increase and the enlarged magnet aperture. Nevertheless, the upgrade from emulsion films to silicon vertex detectors will preserve the efficiency of the experiment even in such a high-rate environment.
- Open Access
- 11 April 2026
- Published by Elsevier in Transportation Research Interdisciplinary Perspectives
- Vol. 37
A framework for resilience assessment of urban transportation systems under seismic hazard
- 11 April 2026
- Published by Elsevier in Transportation Research Interdisciplinary Perspectives
- Vol. 37
Open AccessA framework for resilience assessment of urban transportation systems under seismic hazard
- Open Access
- 1 December 2025
- Published by IOP Publishing in Journal of Instrumentation
- Vol. 20 (12) , T12002
The SND@LHC neutron shielding
This paper presents the design, construction, and simulation-based validation of the ColdBox, a combined neutron shielding and insulating enclosure for the Scattering and Neutrino Detector at the LHC (SND@LHC). The emulsion films in the detector's target region require protection from the intense neutron radiation background and a stable environment of 15 ± 1 °C and 50–55 % relative humidity for long-term stability. The ColdBox meets these requirements through a dual-layer structure: an external 5 cm plexiglass wall to moderate fast neutrons, and an internal 4 cm layer of borated polyethylene (with 35 % boron content) to capture thermal neutrons. The mechanical design, based on a robust aluminum frame, accommodates the constraints of the TI18 tunnel. FLUKA simulations were used to optimize the shielding configuration, showing a significant reduction in the neutron flux, with a simulated ratio of shielded to unshielded thermal neutron fluence of 2.3 × 10 -3 . This result is consistent with initial measurements from BatMon detectors. The design also provides a sealed volume for a cooling system to maintain the required temperature and humidity, ensuring the necessary conditions for the emulsion films' integrity.
- 1 December 2025
- Published by IOP Publishing in Journal of Instrumentation
- Vol. 20 (12) , T12002
Open AccessThe SND@LHC neutron shielding
This paper presents the design, construction, and simulation-based validation of the ColdBox, a combined neutron shielding and insulating enclosure for the Scattering and Neutrino Detector at the LHC (SND@LHC). The emulsion films in the detector's target region require protection from the intense neutron radiation background and a stable environment of 15 ± 1 °C and 50–55 % relative humidity for long-term stability. The ColdBox meets these requirements through a dual-layer structure: an external 5 cm plexiglass wall to moderate fast neutrons, and an internal 4 cm layer of borated polyethylene (with 35 % boron content) to capture thermal neutrons. The mechanical design, based on a robust aluminum frame, accommodates the constraints of the TI18 tunnel. FLUKA simulations were used to optimize the shielding configuration, showing a significant reduction in the neutron flux, with a simulated ratio of shielded to unshielded thermal neutron fluence of 2.3 × 10 -3 . This result is consistent with initial measurements from BatMon detectors. The design also provides a sealed volume for a cooling system to maintain the required temperature and humidity, ensuring the necessary conditions for the emulsion films' integrity.
- 30 October 2025
- Published by Springer Nature
- p. 39-48
A Stochastic Post-disaster Recovery Model for the Healthcare Urban Community of Naples, Italy
- 30 October 2025
- Published by Springer Nature
- p. 39-48
A Stochastic Post-disaster Recovery Model for the Healthcare Urban Community of Naples, Italy
- Open Access
- 6 October 2025
- Published by AIP Publishing in Applied Physics Letters
- Vol. 127 (14)
A postbuckling-based metamaterial for switching the propagation of surface acoustic waves
The use of periodic materials for wave control and signal processing has been a focus of intensive research over the past two decades and continues to garner significant attention. Common signal processing mechanisms like switches and rectifiers often depend on magnetic fields and/or logic gates for their activation. We propose a metamaterial that enables the control of mechanical waves—surface acoustic waves—through an ON–OFF mechanism that switches the propagation of the waves through a tunable platform of elastic beams. In the OFF configuration, the beams remain in their undeformed state and resonate at a specific frequency range, creating a bandgap that stops wave propagation. Conversely, in the ON configuration, the beams undergo buckling, redistributing the vibration energy across multiple modes and eliminating the bandgap, thus allowing wave propagation. Analytical and numerical findings demonstrate the significant potential of this mechanism for controlling wave propagation in nonlinear periodic materials. This switching mechanism relies purely on mechanical processes, thereby eliminating the need for external fields.
- 6 October 2025
- Published by AIP Publishing in Applied Physics Letters
- Vol. 127 (14)
Open AccessA postbuckling-based metamaterial for switching the propagation of surface acoustic waves
The use of periodic materials for wave control and signal processing has been a focus of intensive research over the past two decades and continues to garner significant attention. Common signal processing mechanisms like switches and rectifiers often depend on magnetic fields and/or logic gates for their activation. We propose a metamaterial that enables the control of mechanical waves—surface acoustic waves—through an ON–OFF mechanism that switches the propagation of the waves through a tunable platform of elastic beams. In the OFF configuration, the beams remain in their undeformed state and resonate at a specific frequency range, creating a bandgap that stops wave propagation. Conversely, in the ON configuration, the beams undergo buckling, redistributing the vibration energy across multiple modes and eliminating the bandgap, thus allowing wave propagation. Analytical and numerical findings demonstrate the significant potential of this mechanism for controlling wave propagation in nonlinear periodic materials. This switching mechanism relies purely on mechanical processes, thereby eliminating the need for external fields.
- Open Access
- 3 October 2025
- Published by Springer Nature in Scientific Data
- Vol. 12 (1) , 1-16
Seismic resilience of urban networks: dataset for infrastructure visualization and vulnerability assessment
We provide geographic information system (GIS) data and a multimodal dataset from a systematic infrastructure vulnerability assessment in the urban road networks of Turin and Naples, Italy. The seismic typologies of the relevant structural objects (SOs), including bridges, buildings, and roads, were evaluated using digital elevation models (DEMs) and satellite data. The presented GIS data are essential for visualizing and spatially interconnecting SOs; this enables network modeling as a complex system within the Spatial Data Infrastructure (SDI) portfolio of interest. The dataset also includes landslide characteristics from Geoportale Piemonte and the GeoNetwork catalog. Potential applications include resilience analysis, seismic risk assessment, emergency response planning, and post-disaster recovery estimations. Moreover, the dataset helps investigate the interplay between structural vulnerability and geohazards like landslides, heavy rainfall, and earthquakes. Notably, it is particularly relevant for research on urban networks as complex systems, where SDIs assess transportation efficiency and functionality in both pre- and post-event scenarios.
- 3 October 2025
- Published by Springer Nature in Scientific Data
- Vol. 12 (1) , 1-16
Open AccessSeismic resilience of urban networks: dataset for infrastructure visualization and vulnerability assessment
We provide geographic information system (GIS) data and a multimodal dataset from a systematic infrastructure vulnerability assessment in the urban road networks of Turin and Naples, Italy. The seismic typologies of the relevant structural objects (SOs), including bridges, buildings, and roads, were evaluated using digital elevation models (DEMs) and satellite data. The presented GIS data are essential for visualizing and spatially interconnecting SOs; this enables network modeling as a complex system within the Spatial Data Infrastructure (SDI) portfolio of interest. The dataset also includes landslide characteristics from Geoportale Piemonte and the GeoNetwork catalog. Potential applications include resilience analysis, seismic risk assessment, emergency response planning, and post-disaster recovery estimations. Moreover, the dataset helps investigate the interplay between structural vulnerability and geohazards like landslides, heavy rainfall, and earthquakes. Notably, it is particularly relevant for research on urban networks as complex systems, where SDIs assess transportation efficiency and functionality in both pre- and post-event scenarios.