- 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
- Computational Physics and Python Applications
- Neutrino Physics Research
- Cosmology and Gravitation Theories
- Astrophysics and Cosmic Phenomena
- Particle accelerators and beam dynamics
- Radiation Detection and Scintillator Technologies
- Particle Accelerators and Free-Electron Lasers
- Black Holes and Theoretical Physics
- Distributed and Parallel Computing Systems
- Superconducting Materials and Applications
- Atomic and Subatomic Physics Research
- Radiation Therapy and Dosimetry
- advanced mathematical theories
- Rare-earth and actinide compounds
- Noncommutative and Quantum Gravity Theories
- Nuclear physics research studies
- X-ray Diffraction in Crystallography
- Stochastic processes and financial applications
- Nuclear Physics and Applications
- Medical Imaging Techniques and Applications
Fermi National Accelerator Laboratory
2012-2025
University of Antwerp
2024
A. Alikhanyan National Laboratory
2022-2024
Institute of High Energy Physics
2020-2024
University of Notre Dame
2021
Texas Tech University
1997-2006
University of Nebraska–Lincoln
2000
Children's Defense Fund
2000
Instituto de Física de Cantabria
2000
Universidad de Cantabria
2000
This volume of the LBNF/DUNE Conceptual Design Report cover Long-Baseline Neutrino Facility for DUNE and describes LBNF Project, which includes design construction beamline at Fermilab, conventional facilities both Fermilab SURF, cryostat cryogenics infrastructure required far detector.
The NT-02 neutrino physics target made of the isotropic graphite grade produced neutrinos for MINOS and MINERVA high-energy experiments. segmented, 95-cm-long was bombarded with a 340 kW, Gaussian 1.1 mm sigma beam 120 GeV protons reaching $6.516\ifmmode\times\else\texttimes\fi{}{10}^{20}$ on peak fluence $8.6\ifmmode\times\else\texttimes\fi{}{10}^{21}\text{ }\text{ }\mathrm{protons}/{\mathrm{cm}}^{2}$. Reductions in detected events during experiment were attributed to radiation-induced...
Operating and improving the understanding of Fermilab Accelerator Complex for colliding beam experiments requires advanced software methods tools. The Shot Data Analysis (SDA) has been developed to fulfill this need. from is stored in a relational database, served programs users via Web-based Summary tables are systematically generated during after store. These (the Supertable, Recomputed Emittances, Intensities other tables) discussed here.
In this paper we discuss the luminosity determination at Tevatron. We measurements by machine as well using detectors of CDF and D0 experiments. uncertainties measurements, effort to maximize initial integrated luminosity, challenges lessons learned.
We present the latest measurements on masses, lifetimes and branching fractions for Bs Bc mesons as well b‐baryons. For meson we discuss results mixing. These were produced by CDF D0 experiments at Fermilab or earlier LEP PEPII experiments.
In this brief White Paper we glance over the studies carried out so far by CMS Collaboration in field of conventional and exotic hadron spectroscopy. We highlight most relevant scientific achievements discuss future perspectives engagement.
The Long Baseline Neutrino Experiment (LBNE) will utilize a neutrino beamline facility located at Fermilab to carry out compelling research program in physics. aim beam of neutrinos toward detector placed the Homestake Mine South Dakota, about 1300 km away. are produced as follows: First, protons extracted from MI-10 section Main Injector (60-120 GeV) hit solid target above grade and produce mesons. Then, charged mesons focused by set focusing horns into 250 m long decay pipe, towards far...
The Long Baseline Neutrino Experiment (LBNE) will utilize a neutrino beamline facility located at Fermilab to carry out compelling research program in physics. aim beam of neutrinos toward detector placed the Homestake Mine South Dakota. are produced three-step process. First, protons from Main Injector (60-120 GeV) hit solid target and produce mesons. Then, charged mesons focused by set focusing horns into decay pipe, towards far detector. Finally, that enter pipe neutrinos. parameters were...