Marco Ferrero
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Marco Ferrero has a total of 1000 co-authors. Here are the top co-authors by number of shared publications:
- Roberta Arcidiacono
INFN sezione di Torino
31 shared publications - Federico Siviero
INFN sezione di Torino
27 shared publications - Nicolo Cartiglia
INFN sezione di Torino
27 shared publications - Francesco Moscatelli
INFN Sezione di Perugia
26 shared publications - Robert White
INFN sezione di Torino
20 shared publications - Valentina Sola
INFN sezione di Torino
20 shared publications
Latest Publications
- Open Access
- 13 November 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (9)
Measurement of Z γ production in proton-proton collisions at s = 13.6 TeV and constraints on neutral triple gauge couplings
A measurement of the Z γ production cross section in proton-proton collisions at a center-of-mass energy of 13.6 TeV is presented. Data corresponding to an integrated luminosity of 34.8 fb − 1 , collected by the CMS experiment at the LHC in 2022 are used. Events with an oppositely charged pair of muons or electrons, with an invariant mass corresponding to a Z boson, together with an isolated photon are selected. The measured fiducial cross section for the combined electron and muon channels is 1.896 ± 0.033 ( stat ) ± 0.054 ( syst ) ± 0.006 ( theo ) pb , in agreement with the standard model prediction of 1.922 ± 0.094 pb . Constraints on neutral triple gauge couplings generated by dimension-8 operators in a recently proposed effective field theory framework are determined for the first time.
- 13 November 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (9)
Open AccessMeasurement of Z γ production in proton-proton collisions at s = 13.6 TeV and constraints on neutral triple gauge couplings
A measurement of the Z γ production cross section in proton-proton collisions at a center-of-mass energy of 13.6 TeV is presented. Data corresponding to an integrated luminosity of 34.8 fb − 1 , collected by the CMS experiment at the LHC in 2022 are used. Events with an oppositely charged pair of muons or electrons, with an invariant mass corresponding to a Z boson, together with an isolated photon are selected. The measured fiducial cross section for the combined electron and muon channels is 1.896 ± 0.033 ( stat ) ± 0.054 ( syst ) ± 0.006 ( theo ) pb , in agreement with the standard model prediction of 1.922 ± 0.094 pb . Constraints on neutral triple gauge couplings generated by dimension-8 operators in a recently proposed effective field theory framework are determined for the first time.
- Open Access
- 19 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10)
First measurements of vector boson scattering in W±W± and WZ production in all-leptonic final states at $ \sqrt{s}=13.6 $ TeVA bstract: The production cross sections of W ± W ± and WZ boson pairs in association with two jets in proton-proton collisions are measured at $$ \sqrt{s}=13.6 $$ TeV. The data sample corresponds to an integrated luminosity of 171 fb − 1 , collected with the CMS detector during 2022–2024. The measurements are performed in the leptonic decay modes: W ± Z → ℓ ± νℓ′ ± ℓ′ ∓ and W ± W ± → ℓ ± νℓ′ ± ν , where ℓ , ℓ′ = e or μ . The electroweak productions of W ± W ± and WZ bosons are each observed with a significance greater than five standard deviations from the background-only hypothesis. Differential fiducial cross sections as functions of several observables are also measured.- 19 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10)
Open AccessFirst measurements of vector boson scattering in W±W± and WZ production in all-leptonic final states at $ \sqrt{s}=13.6 $ TeVA bstract: The production cross sections of W ± W ± and WZ boson pairs in association with two jets in proton-proton collisions are measured at $$ \sqrt{s}=13.6 $$ TeV. The data sample corresponds to an integrated luminosity of 171 fb − 1 , collected with the CMS detector during 2022–2024. The measurements are performed in the leptonic decay modes: W ± Z → ℓ ± νℓ′ ± ℓ′ ∓ and W ± W ± → ℓ ± νℓ′ ± ν , where ℓ , ℓ′ = e or μ . The electroweak productions of W ± W ± and WZ bosons are each observed with a significance greater than five standard deviations from the background-only hypothesis. Differential fiducial cross sections as functions of several observables are also measured. - Open Access
- 1 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10)
Measurement of event shape variables using charged particles inside jets in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016–2018, corresponding to an integrated luminosity of 138 fb − 1 . The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the predictions from several models for multijet production. Overall, there is general agreement between several theoretical predictions and the data with scope for improvement of our understanding of QCD at different energy scales.
- 1 October 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (10)
Open AccessMeasurement of event shape variables using charged particles inside jets in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: Event shape variables, constructed from the four-momenta of the final-state objects in an event, are sensitive to the predictions of quantum chromodynamics in multijet production. A measurement of five event shape variables is presented, using proton-proton collision data collected at a centre-of-mass energy of 13 TeV with the CMS detector during 2016–2018, corresponding to an integrated luminosity of 138 fb − 1 . The variables are evaluated using the charged particles inside jets. After correcting for detector effects, their distributions are compared with the predictions from several models for multijet production. Overall, there is general agreement between several theoretical predictions and the data with scope for improvement of our understanding of QCD at different energy scales.
- Open Access
- 6 August 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (8)
Search for a Higgs boson produced in association with a charm quark and decaying to a W boson pair in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: This paper presents a search for a Higgs boson produced in association with a charm quark (cH) which allows to probe the Higgs-charm Yukawa coupling strength modifier κ c . Higgs boson decays to a pair of W bosons are considered, where one W boson decays to an electron and a neutrino, and the other W boson decays to a muon and a neutrino. The data, corresponding to an integrated luminosity of 138 fb − 1 , were collected between 2016 and 2018 with the CMS detector at the LHC at a center-of-mass energy of $$ \sqrt{s}=13 $$ TeV. Upper limits at the 95% confidence level (CL) are set on the ratio of the measured yield to the standard model expectation for cH production. The observed (expected) upper limit is 1065 (506), corresponding to an observed (expected) constraint of |κ c | < 211 (95). When combined with the previous search for cH in the diphoton decay channel of the Higgs boson, the limits are interpreted as observed (expected) constraints at 95% CL on the value of κ c , |κ c | < 47 (51).- 6 August 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (8)
Open AccessSearch for a Higgs boson produced in association with a charm quark and decaying to a W boson pair in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: This paper presents a search for a Higgs boson produced in association with a charm quark (cH) which allows to probe the Higgs-charm Yukawa coupling strength modifier κ c . Higgs boson decays to a pair of W bosons are considered, where one W boson decays to an electron and a neutrino, and the other W boson decays to a muon and a neutrino. The data, corresponding to an integrated luminosity of 138 fb − 1 , were collected between 2016 and 2018 with the CMS detector at the LHC at a center-of-mass energy of $$ \sqrt{s}=13 $$ TeV. Upper limits at the 95% confidence level (CL) are set on the ratio of the measured yield to the standard model expectation for cH production. The observed (expected) upper limit is 1065 (506), corresponding to an observed (expected) constraint of |κ c | < 211 (95). When combined with the previous search for cH in the diphoton decay channel of the Higgs boson, the limits are interpreted as observed (expected) constraints at 95% CL on the value of κ c , |κ c | < 47 (51). - Open Access
- 6 August 2026
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 1092
Periphery layout strategies to mitigate discharges in thin silicon sensors
- 6 August 2026
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 1092
Open AccessPeriphery layout strategies to mitigate discharges in thin silicon sensors
- Open Access
- 1 June 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (6)
Search for dark matter production in association with bottom quarks and a lepton pair in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search is performed for dark matter produced in association with bottom quarks and a pair of electrons or muons in data collected with the CMS detector at the LHC, corresponding to 138 fb − 1 of integrated luminosity of proton-proton collisions at a center-of-mass energy of 13 TeV. For the first time at the LHC, the associated production of a bottom quark-antiquark pair and a new heavy neutral Higgs boson (H) that subsequently decays into a leptonically decaying Z boson and a pseudoscalar (a) is explored. The latter acts as a dark matter mediator in the context of the two Higgs doublet model plus a pseudoscalar (2HDM+a). Multivariate techniques that target a wide range of mass configurations for the H and a particles are used. The observations are consistent with the expectations from standard model processes. Upper limits at 95% confidence level are set on the product of cross section and branching fraction of the new particles, ranging from 10 − 2 pb for an H mass of 400 GeV to 10 − 3 pb for an H mass of 2000 GeV. Constraints on the parameter space of a benchmark 2HDM+a model are derived and compared with expectations in the context of cosmological predictions.
- 1 June 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (6)
Open AccessSearch for dark matter production in association with bottom quarks and a lepton pair in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search is performed for dark matter produced in association with bottom quarks and a pair of electrons or muons in data collected with the CMS detector at the LHC, corresponding to 138 fb − 1 of integrated luminosity of proton-proton collisions at a center-of-mass energy of 13 TeV. For the first time at the LHC, the associated production of a bottom quark-antiquark pair and a new heavy neutral Higgs boson (H) that subsequently decays into a leptonically decaying Z boson and a pseudoscalar (a) is explored. The latter acts as a dark matter mediator in the context of the two Higgs doublet model plus a pseudoscalar (2HDM+a). Multivariate techniques that target a wide range of mass configurations for the H and a particles are used. The observations are consistent with the expectations from standard model processes. Upper limits at 95% confidence level are set on the product of cross section and branching fraction of the new particles, ranging from 10 − 2 pb for an H mass of 400 GeV to 10 − 3 pb for an H mass of 2000 GeV. Constraints on the parameter space of a benchmark 2HDM+a model are derived and compared with expectations in the context of cosmological predictions.
- Open Access
- 19 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3)
Search for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search for signatures of a dark analog to quantum chromodynamics is performed. The analysis targets long-lived dark mesons that decay into standard-model particles, with a high branching fraction of the dark mesons decaying into muons. The dark mesons are formed by the hadronisation of dark partons, which are produced by a decay of the Higgs boson. The search is performed using a data set corresponding to an integrated luminosity of 41.6 fb − 1 , which was collected in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV by the CMS experiment at the CERN LHC in 2018 using non-prompt muon triggers. The search is based on resonant muon pair signatures. Machine-learning techniques are employed in the analysis, utilising boosted decision trees to discriminate between signal and background. No significant excess is observed above the standard model expectation. Upper limits on the branching fraction of the Higgs boson decaying to dark partons are determined to be as low as 10 − 4 at 95% confidence level, surpassing and extending the existing limits on models with dark $$ \overset{\sim }{\upomega} $$ mesons for mean proper decay lengths of less than 500 mm and for $$ \overset{\sim }{\upomega} $$ masses down to 0.3 GeV. First limits are set for extended dark-shower models with two dark flavours that contain dark photons, probing their masses down to 0.33 GeV.- 19 March 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (3)
Open AccessSearch for low-mass hidden-valley dark showers with non-prompt muon pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeVA bstract: A search for signatures of a dark analog to quantum chromodynamics is performed. The analysis targets long-lived dark mesons that decay into standard-model particles, with a high branching fraction of the dark mesons decaying into muons. The dark mesons are formed by the hadronisation of dark partons, which are produced by a decay of the Higgs boson. The search is performed using a data set corresponding to an integrated luminosity of 41.6 fb − 1 , which was collected in proton-proton collisions at $$ \sqrt{s}=13 $$ TeV by the CMS experiment at the CERN LHC in 2018 using non-prompt muon triggers. The search is based on resonant muon pair signatures. Machine-learning techniques are employed in the analysis, utilising boosted decision trees to discriminate between signal and background. No significant excess is observed above the standard model expectation. Upper limits on the branching fraction of the Higgs boson decaying to dark partons are determined to be as low as 10 − 4 at 95% confidence level, surpassing and extending the existing limits on models with dark $$ \overset{\sim }{\upomega} $$ mesons for mean proper decay lengths of less than 500 mm and for $$ \overset{\sim }{\upomega} $$ masses down to 0.3 GeV. First limits are set for extended dark-shower models with two dark flavours that contain dark photons, probing their masses down to 0.33 GeV. - Open Access
- 13 March 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (5)
Characterization of the quantum state of top quark pairs produced in proton-proton collisions at s = 13 TeV using the beam and helicity bases
Measurements of the spin correlation coefficients in the beam basis are presented for top quark-antiquark ( t t ¯ ) systems produced in proton-proton collisions at s = 13 TeV collected by the CMS experiment in 2016–2018, and corresponding to an integrated luminosity of 138 fb − 1 . The t t ¯ system is reconstructed from final states containing an electron or muon and jets. Together with the previously reported results in the helicity basis, these measurements are used to decompose the system into the Bell and spin eigenstates in various kinematic regions. The spin correlation coefficients are also used to evaluate properties of the t t ¯ quantum state, such as the purity, von Neumann entropy, and entanglement. All results are consistent with standard model predictions.
- 13 March 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 113 (5)
Open AccessCharacterization of the quantum state of top quark pairs produced in proton-proton collisions at s = 13 TeV using the beam and helicity bases
Measurements of the spin correlation coefficients in the beam basis are presented for top quark-antiquark ( t t ¯ ) systems produced in proton-proton collisions at s = 13 TeV collected by the CMS experiment in 2016–2018, and corresponding to an integrated luminosity of 138 fb − 1 . The t t ¯ system is reconstructed from final states containing an electron or muon and jets. Together with the previously reported results in the helicity basis, these measurements are used to decompose the system into the Bell and spin eigenstates in various kinematic regions. The spin correlation coefficients are also used to evaluate properties of the t t ¯ quantum state, such as the purity, von Neumann entropy, and entanglement. All results are consistent with standard model predictions.
- Open Access
- 1 February 2026
- Published by IOP Publishing in Journal of Instrumentation
- Vol. 21 (02) , C02022
Measurements and radiation damage modelling of small-pitch 3D pixel detectors at high fluences
The macroscopic electrical response of small-pitch50 × 50 μm 2 3D pixel sensors was investigated by comparing experimental measurements with TCAD simulations. Selected trap parameters (introduction rates and capture cross sections) of the CERN (Folkestad) model, originally developed for fluences up to 8 × 10 15 n eq /cm 2 , were varied to study their impact on the simulated characteristics and to assess the sensitivity in reproducing the measured behaviour. The analysis focuses on the I-V, C-V, and charge collection efficiency (CCE) characteristics at fluences of 1 × 10 16 n eq /cm 2 and 2.5 × 10 16 n eq /cm 2 . This work highlights how variations in trap parameters influence the performance of irradiated 3D sensors and supports the extension of the CERN model for 3D detectors operating at high fluence.
- 1 February 2026
- Published by IOP Publishing in Journal of Instrumentation
- Vol. 21 (02) , C02022
Open AccessMeasurements and radiation damage modelling of small-pitch 3D pixel detectors at high fluences
The macroscopic electrical response of small-pitch50 × 50 μm 2 3D pixel sensors was investigated by comparing experimental measurements with TCAD simulations. Selected trap parameters (introduction rates and capture cross sections) of the CERN (Folkestad) model, originally developed for fluences up to 8 × 10 15 n eq /cm 2 , were varied to study their impact on the simulated characteristics and to assess the sensitivity in reproducing the measured behaviour. The analysis focuses on the I-V, C-V, and charge collection efficiency (CCE) characteristics at fluences of 1 × 10 16 n eq /cm 2 and 2.5 × 10 16 n eq /cm 2 . This work highlights how variations in trap parameters influence the performance of irradiated 3D sensors and supports the extension of the CERN model for 3D detectors operating at high fluence.