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The Australian Synchrotron is a 3 GeV national synchrotron radiation facility located in Clayton, ... The linear accelerator (or linac) uses a series of RF cavities ...
A linear particle accelerator (often shortened to linac) is a type of particle accelerator that accelerates charged subatomic particles or ions to a high speed by subjecting them to a series of oscillating electric potentials along a linear beamline.
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 [7] 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 remains of the RSPhysSE 500MJ homopolar generator 2 MeV "High Voltage" Van de Graaff linear accelerator built in 1960. Sir Mark Oliphant was the founder of the school and its first director from 1950 to 1963. The school was originally called the "Research School of Physical Sciences" with "Engineering" being added to its title in 1990 to ...
The first synchrotron to use the "racetrack" design with straight sections, a 300 MeV electron synchrotron at University of Michigan in 1949, designed by Dick Crane.. A synchrotron is a particular type of cyclic particle accelerator, descended from the cyclotron, in which the accelerating particle beam travels around a fixed closed-loop path.
The longest linac in the world is the Stanford Linear Accelerator, SLAC, which is 3 km (1.9 mi) long. SLAC was originally an electron–positron collider but is now a X-ray Free-electron laser. Linear high-energy accelerators use a linear array of plates (or drift tubes) to which an alternating high-energy field is applied.
An energy recovery linac (ERL) is a type of linear particle accelerator that provides a beam of electrons used to produce x-rays by synchrotron radiation. [1] First proposed in 1965 [ 2 ] the idea gained interest since the early 2000s.
A radio-frequency quadrupole (RFQ) is a linear accelerator component [1] generally used at low beam energies, roughly 2keV [2] to 3MeV. It is similar in layout to a quadrupole mass analyser but its purpose is to accelerate a single-species beam (a beam of one particular type of particle) rather than perform mass spectrometry on a multiple-species beam.