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Accelerator-driven subcritical reactor. An accelerator-driven subcritical reactor (ADSR) is a nuclear reactor design formed by coupling a substantially subcritical nuclear reactor core with a high-energy proton or electron accelerator. It could use thorium as a fuel, which is more abundant than uranium. [1]
Dates of operation. 1966–2006. Succeeded by. LCLS. SLAC National Accelerator Laboratory, originally named the Stanford Linear Accelerator Center, [2] [3] is a federally funded research and development center in Menlo Park, California, United States. Founded in 1962, the laboratory is now sponsored by the United States Department of Energy and ...
Fermitron was an accelerator sketched by Enrico Fermi on a notepad in the 1940s proposing an accelerator in stable orbit around the Earth. The undulator radiation collider is a design for an accelerator with a center-of-mass energy around the GUT scale. It would be light-weeks across and require the construction of a Dyson swarm around the Sun.
The Superconducting Super Collider ( SSC) (also nicknamed the "Desertron" [2]) was a particle accelerator complex under construction in the vicinity of Waxahachie, Texas, United States. Its planned ring circumference was 87.1 kilometers (54.1 mi) with an energy of 20 TeV per proton and was designed to be the world's largest and most energetic ...
Here the plasma accelerator science provides the breakthrough to generate, sustain, and exploit the highest fields ever produced by science in the laboratory. Wake created by an electron beam in a plasma. The acceleration gradient produced by a plasma wake is in the order of the wave breaking field, which is.
The high voltage generator is right, the ion source and beam tube is at left. An electrostatic particle accelerator is a particle accelerator in which charged particles are accelerated to a high energy by a static high voltage potential. This contrasts with the other major category of particle accelerator, oscillating field particle ...
v. t. e. In physics, the Heisenberg picture or Heisenberg representation [1] is a formulation (largely due to Werner Heisenberg in 1925) of quantum mechanics in which the operators ( observables and others) incorporate a dependency on time, but the state vectors are time-independent, an arbitrary fixed basis rigidly underlying the theory.
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