Mihail Bogdan Blidaru
A5020290764- High-Energy Particle Collisions Research
- Particle physics theoretical and experimental studies
- Quantum Chromodynamics and Particle Interactions
- Particle Detector Development and Performance
- Nuclear reactor physics and engineering
- Dark Matter and Cosmic Phenomena
- Statistical Methods and Bayesian Inference
- Nuclear physics research studies
- CCD and CMOS Imaging Sensors
- Stochastic processes and statistical mechanics
- Cosmology and Gravitation Theories
- Radiation Detection and Scintillator Technologies
- Advanced Semiconductor Detectors and Materials
- Computational Physics and Python Applications
- Pediatric Urology and Nephrology Studies
- Superconducting Materials and Applications
- Black Holes and Theoretical Physics
- Particle Accelerators and Free-Electron Lasers
- Muon and positron interactions and applications
- Atomic and Molecular Physics
- Theoretical and Computational Physics
- Pulsars and Gravitational Waves Research
GSI Helmholtz Centre for Heavy Ion Research
2021-2025
A. Alikhanyan National Laboratory
2021-2024
Financiadora de Estudos e Projetos
2023
National Nuclear Research Center
2023
National Council for Scientific and Technological Development
2023
Technical University of Munich
2021
Bent monolithic active pixel sensors are the basis for planned fully cylindrical ultra low material budget tracking detector ITS3 of ALICE experiment. This paper presents results from testbeam campaigns using high-energy particles to verify performance 50 um thick bent ALPIDE chips in terms efficiency and spatial resolution. The were radii 18, 24 30 mm, slightly smaller than foreseen bending future layers. An larger $99.9\%$ a resolution approximately 5 um, line with nominal operation flat...
Analogue test structures were fabricated using the Tower Partners Semiconductor Co. CMOS 65 nm ISC process. The purpose was to characterise and qualify this process optimise sensor for next generation of Monolithic Active Pixels Sensors high-energy physics. technology explored in several variants which differed by: doping levels, pixel geometries pitches (10-25 $\mu$m). These have been tested following exposure varying levels irradiation up 3 MGy $10^{16}$ 1 MeV n$_\text{eq}$ cm$^{-2}$. Here...