searches and limits on new physics
Most of the time, the headline from a frontier experiment is not 'we found something' but 'we did not find it — and here is exactly how hard we looked'. That second result is genuinely valuable. If you fish a lake thoroughly and catch no monster, you have not proven the lake is empty, but you have proven any monster must be smaller or rarer than your net would have caught. Searches and limits are the systematic version of this: hunting for predicted new particles, and when none appear, stating precisely what has been ruled out.
Concretely, a search compares the collisions or events you actually saw against the smooth, well-understood background the Standard Model predicts, and asks whether a hypothesised new particle would have produced a noticeable excess — a bump in a mass spectrum, an unusual spray of missing energy, a rare decay. If the data match the background within their statistical wobble, you set a limit: you can say, with stated confidence, that the new particle either does not exist below some mass or couples more weakly than some value. These limits are usually drawn as exclusion curves carving away regions of possibility.
This matters because it is how the field has actually progressed lately. There is no confirmed physics beyond the Standard Model, so nearly all the results from the Large Hadron Collider and from dark-matter detectors are limits, and they have steadily squeezed supersymmetry, WIMPs, extra dimensions and the rest into ever-smaller corners. A limit is not a failure; it tells theorists which ideas are dead, which survive, and where to point the next, more sensitive experiment. Progress by exclusion is slow but real.
After years of data the LHC could announce: 'we exclude a gluino lighter than about 2,200 GeV at 95% confidence' — meaning if that superpartner existed below that mass, the expected collisions would have shown up, and they did not.
A null result, stated precisely, is a real measurement — an exclusion limit.
A limit never proves a particle does not exist; it only says that if it exists, it must be heavier or more weakly coupled than the experiment could probe. The particle could still be hiding just out of reach.