a factor lighter than the protons or neutrons that made up ordinary matter. A new collection of particles called Sigma, Xi and Lambda baryons had masses larger than the proton and neutron and often decayed into protons or neutrons.
Often particles with very similar masses got the same Greek names. Indeed, the proton and neutron have such similar masses that they were believed to be intimately related, so much so that the German physicist Werner Heisenberg (whose ideas will be at the heart of the next Edge) rechristened them nucleons. But mass was a rather rough and ready way of sorting these particles. Physicists were on the lookout for something more fundamental: a pattern as effective as the one Mendeleev had discovered to order atoms.
The key to finding patterns to make sense of the onslaught of new particles was a new property called strangeness. The name arose due to the rather strange behaviour demonstrated by some of these new particles as they decayed. Since mass is equivalent to energy via Einstein’s equation E=mc2, and nature favours low-energy states, particles with larger mass often try to find ways to decay into particles with smaller mass.
There are several mechanisms for this decay, each depending on one of the fundamental forces. Each mechanism has a characteristic signature which helps physicists to understand which fundamental force is causing the decay. Again it’s energy considerations that control which is the most likely force at work in any particle decay. The strong nuclear force is usually the first to have a go at decaying a particle, and this will generally decay the particle within 10–24 of a second. Next in the hierarchy is the electromagnetic force, which might result in the emission of photons. The weak nuclear force is the most costly in energy terms and so takes longer. A particle that decays via the weak nuclear force is likely to take 10–11 seconds before it decays. So by observing the time it takes to decay, scientists can get some indication of which force is at work.
For example, a Delta baryon decays in 6 × 10–24 seconds to a proton and a pion via the strong nuclear force, while a Sigma baryon takes 8 × 10–11 seconds to decay to the same proton and pion. The longer time of decay indicates that it is controlled by the weak nuclear force. In the middle we have the example of a neutrally charged pion decaying via the electromagnetic force into two photons, which happens in 8.4 × 10–17 seconds.
Imagine a ball sitting in a valley. There is a path to the right which, with a little push, will take the ball over the hill into a lower valley. This path corresponds to the strong nuclear force. To the left is a higher hill which is also a path to a lower energy state. This direction represents the work of the weak nuclear force.
A Delta baryon ∆ decays via the strong nuclear force to a proton and a pion. In contrast, a Sigma baryon ∑ decays via the weak nuclear force.
So why did the Delta baryon find a way over the easy hill while the Sigma baryon went the long way? This seemed rather strange. There appeared to be certain particles that encountered a barrier (represented in the figure by a broken line) that prevented them from crossing via the easy route to the lower valley.
THERE IS NO EXQUISITE BEAUTY WITHOUT STRANGENESS
The physicists Abraham Pais, Murray Gell-Mann and Kazuhiko Nishijima came up with a cunning strategy to solve this puzzle. They proposed a new property like charge that mediated the way these particles interacted or didn’t interact with the strong nuclear force. This new property, called strangeness, gave physicists a new way to classify all these new particles. Each new particle was given a measure of strangeness according to whether or not its decay would have to take the long route.
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