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High-energy-density physics: foundation of inertial fusion and experimental astrophysics
Contemporary physics (Print), 2018The birth of the closest naked-eye supernova in four centuries on 23 February 1987 had gone unnoticed until Ian Shelton discovered an extra star in the photographic plate he was developing early the next morning. SN 1987A, as the supernova has come to be
B. Ishak
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Grid applications for high energy physics experiments
The 6th IEEE/ACM International Workshop on Grid Computing, 2005., 2005This paper discusses the use of e-science grid in providing computational resources for modern international high energy physics (HEP) experiments. We investigate the suitability of the current generation of grid software to provide the necessary resources to perform large-scale simulation of the experiment and analysis of data in the context of ...
A. Khan+19 more
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Design of a high throughput electronics module for high energy physics experiments
, 2016High-energy physics experiments enable us to explore and understand particle properties and interactions. An increase in luminosity in the accelerator, which allows us to study particles in higher energy ranges, demands faster data transmission and ...
王春杰, 刘振安, 赵京周, 刘兆
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EMC Planning for High-Energy Physics Experiments
IEEE Transactions on Electromagnetic Compatibility, 2016During the last years, the large hadron collider (LHC), the most powerful particle accelerator in the world, has been running at CERN in Geneva, Switzerland. It includes four large high-energy experiments and the compact muon solenoid (CMS) is one of them. The electronic read-out for the CMS experiment is designed to process signals in the range of $\
F. Arteche+2 more
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Trigger control in a high energy physics experiment
IEEE Transactions on Nuclear Science, 1989Control and diagnostic tools for the event-filtering system (trigger) of the L3 experiment at the LEP (Large Electron Positron) collider have been implemented using an expert system. The structure and behavior of the trigger electronics has been modeled using the hybrid framework (allowing both frame-based design and rule-based reasoning) of the shell ...
F. Menczer+3 more
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Introduction to Ultrahigh Energy Cosmic Ray Physics
, 2020Cosmic ray physics has recently attracted a great deal of attention from the high energy physics community because of the discovery of new sources and the advent of new techniques.
P. Sokolsky
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, 2008
When searching for new phenomena in high-energy physics, statistical analysis is complicated by the presence of nuisance parameters, representing uncertainty in the physics of interactions or in detector properties.
Radford M. Neal
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When searching for new phenomena in high-energy physics, statistical analysis is complicated by the presence of nuisance parameters, representing uncertainty in the physics of interactions or in detector properties.
Radford M. Neal
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Photomultiplier Counters in High-Energy Physics Experiments
IRE Transactions on Nuclear Science, 1956Techniques in the use of photomultipliers in high-energy nuclear physics are presented by the description of experiments that have been prominent recently. The applications involve the use of photomultipliers with attendant amplification at the limit of present possibilities of time resolution.
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Experiments in high energy physics: A brief introduction
2008A brief description of a “standard” High Energy Physics experiment focussing on what are the main measurements and how they are obtained is herein reported. The historical example of the discovery of neutral currents by the Gargamelle experiment in 1973 is presented to show the long path between the data collection and the final results.
Mário Pimenta, Lip, Ist
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Moderate energy ions for high energy density physics experiments
Physics of Plasmas, 2004This paper gives the results of a preliminary exploration of whether moderate energy ions (≈0.3–3 MeV/amu) could be useful as modest-cost drivers for high energy density physics experiments. It is found that if the target thickness is chosen so that the ion beam enters and then leaves the target in the vicinity of the peak of the dE/dX (stopping power)
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