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History
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An overview graphic of the planned ILC based on the accelerator design of the Technical Design Report
An overview graphic of the planned ILC based on the accelerator design of the Technical Design Report
A niobium-based 1.3 GHz nine-cell superconducting radio frequency cavity to be used at the main linac
A niobium-based 1.3 GHz nine-cell superconducting radio frequency cavity to be used at the main linac
An interior view of the niobium superconducting radio frequency cavity
An interior view of the niobium superconducting radio frequency cavity
A cryomodule being tested at Fermilab
A cryomodule being tested at Fermilab
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The linac within the Australian Synchrotron uses radio waves from a series of RF cavities at the start of the linac to accelerate the electron beam in
The linac within the Australian Synchrotron uses radio waves from a series of RF cavities at the start of the linac to accelerate the electron beam in bunches to energies of 100 MeV.
Alvarez type linac
Alvarez type linac
Quadrupole magnets surrounding the linac of the Australian Synchrotron are used to help focus the electron beam
Quadrupole magnets surrounding the linac of the Australian Synchrotron are used to help focus the electron beam
The Stanford University superconducting linear accelerator, housed on campus below the Hansen Labs until 2007. This facility is separate from SLAC
The Stanford University superconducting linear accelerator, housed on campus below the Hansen Labs until 2007. This facility is separate from SLAC