The sun sets on SATURNE
After a 40-year career, first as a weak focusing machine and then rebuilt with strong focusing, the French SATURNE synchrotron has exited the physics stage.
Thank you for registering
If you'd like to change your details at any time, please visit My account
After a 40-year career, first as a weak focusing machine and then rebuilt with strong focusing, the French SATURNE synchrotron has exited the physics stage.
Shortly after the dedication of the PEP-II B-Factory at the Stanford Linear Accelerator Centre on 26 October, a team led by John Seeman resumed the task of commissioning the new electronpositron co...
Spearheading the construction effort for CERN's LHC collider is the groundwork for the 1232 superconducting dipole magnets, to be cooled by superfluid helium at 1.9K. Material procurement and tooling...
The invention and development of electron cooling by Gersh Budker's team in Novosibirsk in the late 1960s and early 1970s set physics on a new route to discovery. Electron cooling has become crucial f...
The 1998 EPS-IGA prize for outstanding work in the accelerator field was awarded to CERN’s Cris Benvenuti for “major breakthroughs in achieving ultra-high vacua in storage rings”.
International partners are being sought for the AUSTRON, a proposal for a pulsed high-flux neutron spallation source which could provide an international research centre in central Europe. Austria ha...
After achieving its first electronpositron collisions this summer, the PEP-II B-Factory at the Stanford Linear Accelerator Center was formally dedicated on 23 October.
A recent celebration in the assembly area at Brookhaven's RHIC Magnet Facility marked the completion of magnet production for the laboratory's RHIC Relativistic Heavy Ion Collider.
On 24 September, US Energy Secretary Bill Richardson put the finishing touches to the installation of the 366th and final 20-ton dipole magnet to steer the beams in Fermilab's new 150 GeV, 2.25 mile...
Smooth running at CERN's LEP electronpositron collider, now at 189 GeV collision energy (94.5 GeV per beam), is reflected in a fast climbing, integrated luminosity curve.