A panoramic view of the PHENIX detector's building and counting house. To the left, an entrance to RHIC's particle beam ring is visible. When access is required, the enormous concrete slabs that block the entrance are removed with a crane to expose the route into the tunnel.
The Relativistic Heavy Ion Collider (RHIC) at Brookhaven is a medium-to-high-energy machine that plays a unique role in the study of the early universe. While most particle accelerators collide single particles (like protons and antiprotons in the case Fermilab’s Tevatron), RHIC’s main purpose is to collide gold nuclei, each of which contains 79 protons.
Why the additional mass? The results of a proton-antiproton collision usually look something like this:
A proton-antiproton collision at the Tevatron (courtesy of Rockefeller University/CDF)
Gold ion collisions produce tracks like this:
A gold ion collision at RHIC (courtesy of RHIC, found on Wikipedia)
Brookhaven’s National Synchrotron Light Source, we would discover, is just that — a light source. And despite the differences in scale and the methods of production, it isn’t so different from the studio lights used by photographers. In each case, the way to get the best image is to shine a really bright light on the subject and take a picture of it. Indeed, the only respect in which the light source’s name can be misleading is that it does not confine itself to the visible light spectrum, but uses everything between infrared and x-rays.
A view of the workspaces surrounding the smaller ring at Brookhaven's National Synchrotron Light Source
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