S. Zucchelli
A5065883452- Particle physics theoretical and experimental studies
- Quantum Chromodynamics and Particle Interactions
- High-Energy Particle Collisions Research
- Particle Detector Development and Performance
- Neutrino Physics Research
- Dark Matter and Cosmic Phenomena
- Computational Physics and Python Applications
- Particle Accelerators and Free-Electron Lasers
- Medical Imaging Techniques and Applications
- Black Holes and Theoretical Physics
- Superconducting Materials and Applications
- Radiation Detection and Scintillator Technologies
- Astrophysics and Cosmic Phenomena
- Atomic and Subatomic Physics Research
- Cosmology and Gravitation Theories
- Nuclear physics research studies
- Distributed and Parallel Computing Systems
- Stochastic processes and statistical mechanics
- Nuclear Physics and Applications
- International Science and Diplomacy
- Pulsars and Gravitational Waves Research
- Superconducting and THz Device Technology
- Cold Atom Physics and Bose-Einstein Condensates
- Advanced X-ray Imaging Techniques
- Muon and positron interactions and applications
Istituto Nazionale di Fisica Nucleare, Sezione di Bologna
1993-2024
University of Bologna
2009-2024
Istituto Nazionale di Fisica Nucleare
2005-2024
University of Cagliari
2023
University of California, Los Angeles
2005-2014
National and Kapodistrian University of Athens
2014
Kyungpook National University
2004-2011
Jeonbuk National University
2011
Texas A&M University
2011
Sungkyunkwan University
2011
We have measured \ensuremath{\rho}, the ratio of real to imaginary part p\ifmmode\bar\else\textasciimacron\fi{}p forward elastic-scattering amplitude, at \ensuremath{\surd}s =1.8 TeV. Our result, \ensuremath{\rho}=0.140\ifmmode\pm\else\textpm\fi{}0.069, is compared with extrapolations from lower-energy data based on dispersion relations, and UA4 value =546 GeV.
We have measured the antiproton-proton total cross section at \ensuremath{\surd}s =1.8 TeV Fermilab Tevatron Collider; value obtained is 78.3\ifmmode\pm\else\textpm\fi{}5.9 mb. B, nuclear slope parameter for elastic scattering, was to be 16.3\ifmmode\pm\else\textpm\fi{}0.5 (GeV/c${)}^{\mathrm{\ensuremath{-}}2}$. From these data, we derive a section.
We have studied proton-antiproton elastic scattering at $\sqrt{s}=1800$ GeV the Fermilab Collider, in range $0.02<|t|<0.13$ ${(\mathrm{G}\mathrm{e}\mathrm{V}/\mathit{c})}^{2}$. Fitting distribution by $\mathrm{exp}(\ensuremath{-}B|t|)$, we obtain a value of $B$ 17.2\ifmmode\pm\else\textpm\fi{}1.3 ${(\mathrm{G}\mathrm{e}\mathrm{V}/\mathit{c})}^{\ensuremath{-}2}$.
Measurements are presented of short range three-particle rapidity correlation in pp interactions at c.m. energies [Formula: see text], 44 and 62 GeV. The data were obtained the CERN Intersecting Storage Rings (ISR) using Split Field Magnet Detector (SFM) with a minimum bias trigger. Three-particle correlations observed for (-+-) (+-+) combinations; no short-range is (---) (+++) configurations. approximately same as two-particle correlations.
Abstract State-of-the-art physics experiments require high-resolution, low-noise, and low-threshold detectors to achieve competitive scientific results. However, experimental environments invariably introduce sources of noise, such as electrical interference or microphonics. The this environmental noise can often be monitored by adding specially designed “auxiliary devices” (e.g. microphones, accelerometers, seismometers, magnetometers, antennae). A model then constructed predict the...
The innermost layer (L00) of the Run IIa silicon detector CDF was planned to be replaced for high luminosity Tevatron upgrade IIb. This new (L0) is designed a radiation tolerant replacement otherwise very similar L00 from IIa. data are read out via long, fine-pitch, low-mass cables allowing hybrids with chips sit at higher z(/spl sim/70 cm), outside tracking volume. design and first results prototyping phase presented. Special focus placed on amount structure induced noise as well...
State-of-the-art physics experiments require high-resolution, low-noise, and low-threshold detectors to achieve competitive scientific results. However, experimental environments invariably introduce sources of noise, such as electrical interference or microphonics. The this environmental noise can often be monitored by adding specially designed "auxiliary devices" (e.g. microphones, accelerometers, seismometers, magnetometers, antennae). A model then constructed predict the detector based...