LHC magnets pass two milestones
The new year at CERN has seen good news for two types of magnet that will be essential to focusing beams in the Large Hadron Collider (LHC).
Thank you for registering
If you'd like to change your details at any time, please visit My account
The new year at CERN has seen good news for two types of magnet that will be essential to focusing beams in the Large Hadron Collider (LHC).
The Linac Coherent Light Source (LCLS) project at the Stanford Linear Accelerator Center (SLAC), which passed the US Department of Energy's "Critical Decision 1" process in October 2002, has been allo...
The nominal parameters for the compact linear collider (CLIC) foresee acceleration of the electron and positron bunches to an energy of 1.5 TeV by 30 GHz normal-conducting accelerating structures oper...
Like all experimental groups around the world, the Belle collaboration at Japan's KEK laboratory is always pushing for higher luminosity, and for the past couple of years the KEKB accelerator team has...
At the Jefferson Laboratory (JLab) in Virginia, US, a multilaboratory team using beams of relativistic electrons has generated broadband terahertz radiation at nearly 20 W average power, several order...
The directors of the two laboratories signed a memorandum of understanding describing the exchange of personnel, equipment, research results and data.
Superconducting (SC) RF cavities are becoming common in accelerators for high-energy and nuclear physics, and the technologies needed to obtain high fields and high-quality factors in elliptical cavit...
It's taken a while, but the world's highest-energy accelerator is back. Fermilab's Tevatron proton-antiproton collider is once again exploring the high-energy frontier, with newly upgraded detectors a...
Brookhaven's Relativistic Heavy Ion Collider (RHIC) began its cool-down on 1 November ready for the first injection of beam in December.
This year, the Beijing Spectrometer (BES) experiment running at the Beijing Electron Positron Collider (BEPC) completed a run at the energy of the y(2S) resonance.