J. Berenguer Antequera
- Particle physics theoretical and experimental studies
- High-Energy Particle Collisions Research
- Quantum Chromodynamics and Particle Interactions
- Particle Detector Development and Performance
- Dark Matter and Cosmic Phenomena
- Cosmology and Gravitation Theories
- Neutrino Physics Research
- Computational Physics and Python Applications
- International Science and Diplomacy
- Black Holes and Theoretical Physics
- Particle Accelerators and Free-Electron Lasers
- Radiation Detection and Scintillator Technologies
- Medical Imaging Techniques and Applications
- Terahertz technology and applications
- Luminescence Properties of Advanced Materials
- Earth Systems and Cosmic Evolution
- Fault Detection and Control Systems
- Superconducting Materials and Applications
- Big Data Technologies and Applications
- Nuclear Physics and Applications
- Cold Atom Physics and Bose-Einstein Condensates
- Atomic and Subatomic Physics Research
- Spectroscopy and Laser Applications
- Distributed and Parallel Computing Systems
- Geophysical Methods and Applications
Istituto Nazionale di Fisica Nucleare, Sezione di Torino
2020-2025
Institute of High Energy Physics
2021-2024
A. Alikhanyan National Laboratory
2022-2024
Università degli Studi del Piemonte Orientale “Amedeo Avogadro”
2021-2023
University of Turin
2020-2023
University of Malaya
2022
University of Montenegro
2021
Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas
2014-2017
The International Linear Collider (ILC) is on the table now as a new global energy-frontier accelerator laboratory taking data in 2030s. ILC addresses key questions for our current understanding of particle physics. It based proven technology. Its experiments will challenge Standard Model physics and provide window to look beyond it. This document brings story up date, emphasizing its strong motivation, readiness construction, opportunity it presents US community.
A New QCD facility at the M2 beam line of CERN SPS COMPASS++/AMBER
The CALICE Semi-Digital Hadronic Calorimeter (SDHCAL) prototype, built in 2011, was exposed to beams of hadrons, electrons and muons two short periods 2012 on different beam lines the CERN SPS. prototype with its 48 active layers, made Glass Resistive Plate Chambers their embedded readout electronics, run triggerless power-pulsing mode. performance SDHCAL during test found be very satisfactory an efficiency exceeding 90% for almost all layers. A linear response (within 5%) a good energy...
The COMPASS experiment recently discovered a new isovector resonance-like signal with axial-vector quantum numbers, the $a_1(1420)$, decaying to $f_0(980)\pi$. With mass too close and width smaller than ground state $a_1(1260)$, it was immediately interpreted as light exotic meson, similar $X$, $Y$, $Z$ states in hidden-charm sector. We show that fully matching experimental data is produced by decay of $a_1(1260)$ resonance into $K^\ast(\to K\pi)\bar{K}$ subsequent rescattering through...
In this paper we review the physics opportunities at linear $e^+e^-$ colliders with a special focus on high centre-of-mass energies and beam polarisation, take fresh look various accelerator technologies available or under development and, for first time, discuss how facility equipped technology mature today could be upgraded of tomorrow to reach much higher and/or luminosities. addition, will detectors alternative collider modes, as well beyond-collider experiments R\&D facilities part...
We study the spin-exotic $J^{PC} = 1^{-+}$ amplitude in single-diffractive dissociation of 190 GeV$/c$ pions into $\pi^-\pi^-\pi^+$ using a hydrogen target and confirm $\pi_1(1600) \to \rho(770) \pi$ amplitude, which interferes with nonresonant $1^{-+}$ amplitude. demonstrate that conflicting conclusions from previous studies on these amplitudes can be attributed to different analysis models treatment dependence squared four-momentum transfer we thus reconcile their experimental findings....
The high granularity of the CALICE Semi-Digital Hadronic CALorimeter (SDHCAL) provides capability to reveal track segments present in hadronic showers. These are then used as a tool probe behaviour active layers situ, better reconstruct energy these showers and also distinguish them from electromagnetic ones. In addition, comparison data simulation helps discriminate among different shower models simulation. To extract recorded SDHCAL, Hough Transform is after being adapted presence dense...
Showers produced by positive hadrons in the highly granular CALICE scintillator-steel analogue hadron calorimeter were studied. The experimental data collected at CERN and FNAL for single particles with initial momenta from 10 to 80 GeV/c. response resolution spatial characteristics of shower development proton- pion-induced showers test beam simulations using Geant4 version 9.6 are compared.
The spatial development of hadronic showers in the CALICE scintillator-steel analogue hadron calorimeter is studied using test beam data collected at CERN and FNAL for single positive pions protons with initial momenta range 10–80 GeV/c. Both longitudinal radial are parametrised two-component functions. parametrisation fit to simulations QGSP_BERT FTFP_BERT physics lists from GEANT4 version 9.6. parameters extracted simulated samples compared two types hadrons. response ratio...
We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive $\omega$ meson muoproduction the proton at COMPASS using 160 GeV/$c$ polarised $ \mu ^{+}$ and ^{-}$ beams impinging liquid hydrogen target. The covers range 5.0 GeV/$c^2$ $< W <$ 17.0 GeV/$c^2$, with average kinematics $\langle Q^{2} \rangle=$ 2.1 (GeV/$c$)$^2$, \rangle= 7.6$ p^{2}_{\rm T} \rangle = 0.16$ (GeV/$c$)$^2$. Here, $Q^2$ denotes virtuality exchanged photon, $W$ mass final hadronic system $p_T$...
The CALICE Semi-Digital Hadron Calorimeter (SDHCAL) technological prototype is a sampling calorimeter using Glass Resistive Plate Chamber detectors with three-threshold readout as the active medium. This technology one of two options proposed for hadron International Large Detector Linear Collider. was exposed to beams muons, electrons and pions different energies at CERN Super Proton Synchrotron. To be able study performance such in future experiments it important ensure reliable simulation...
Based on the observation of sizeable target-transverse-spin asymmetries in single-hadron and hadron-pair production Semi-Inclusive measurements Deep Inelastic Scattering (SIDIS), chiral-odd transversity quark distribution functions $h_1^q$ are nowadays well established. Several possible channels to access these were originally proposed. One candidate is measurement polarisation $\Lambda$ hyperons produced SIDIS off transversely polarised nucleons, where transverse struck might be transferred...
In special tests, the active layers of CALICE Digital Hadron Calorimeter prototype, DHCAL, were exposed to low energy particle beams, without being interleaved by absorber plates. The thickness each layer corresponded approximately 0.29 radiation lengths or 0.034 nuclear interaction lengths, defined mostly copper and steel skins detector cassettes. This paper reports on measurements performed with this device in Fermilab test beam positrons range 1 10 GeV. are compared simulations based...
Hadron leptoproduction in Semi-Inclusive measurements of Deep-Inelastic Scattering (SIDIS) on unpolarised nucleons allows one to get information the intrinsic transverse momentum quarks a nucleon and Boer-Mulders function through measurement azimuthal modulations cross section. These were recently measured by HERMES experiment at DESY proton deuteron targets, COMPASS using CERN SPS muon beam $^6$LiD target. In both cases, amplitudes $\cosϕ_h$ $\cos 2ϕ_h$ show strong kinematic dependences for...
The antiparticle-over-particle multiplicity ratio is measured in deep-inelastic scattering for negatively and positively charged kaons and, the first time, antiprotons protons. data were obtained by COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscalar 6LiD target. regime of ensured requiring Q2 > 1 (GeV/c)2 photon virtuality W>5 GeV/c2 invariant mass produced hadronic system. Bjorken-x restricted to range 0.01 0.40. Protons are identified momentum from 20 GeV/c 60...
We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive $ω$ meson muoproduction the proton at COMPASS using 160 GeV/$c$ polarised $ μ^{+}$ and μ^{-}$ beams impinging liquid hydrogen target. The covers range 5.0 GeV/$c^2$ $< W <$ 17.0 GeV/$c^2$, with average kinematics $\langle Q^{2} \rangle=$ 2.1 (GeV/$c$)$^2$, \rangle= 7.6$ p^{2}_{\rm T} \rangle = 0.16$ (GeV/$c$)$^2$. Here, $Q^2$ denotes virtuality exchanged photon, $W$ mass final hadronic system $p_T$...