Salam carried out his Nobel Prize–winning research at the Imperial College of Science and Technology in the 1960s. His hypothetical equations, which demonstrated an underlying relationship between the electromagnetic force and the weak nuclear force, postulated that the weak force must be transmitted by hitherto-undiscovered particles known as weak vector bosons, or W and Z bosons. Weinberg and Glashow reached a similar conclusion using a different line of reasoning. The existence of the W and Z bosons was eventually verified in 1983 by researchers using particle accelerators at CERN.

Weinberg proposed his version of the electroweak theory in 1967. Electromagnetism and the weak force were both known to operate by the interchange of subatomic particles. Electromagnetism can operate at potentially infinite distances by means of massless particles called photons, while the weak force operates only at subatomic distances by means of massive particles called bosons. Weinberg was able to show that despite their apparent dissimilarities, photons and bosons are actually members of the same family of particles. His work, along with that of Glashow and Salam, made it possible to predict the outcome of new experiments in which elementary particles are made to impinge on one another. An important series of experiments in 1982–83 found strong evidence for the W and Z particles predicted by these scientists’ electroweak theory.

In the 1960s Weinberg and Salam had each independently devised a theory by which the weak nuclear force and the electromagnetic force could be conceived as manifestations of a single unified force called the electroweak force. Their theory could be applied only to leptons, however, a class of particles that includes electrons and neutrinos. Glashow found a way to extend their theory to other classes of elementary particles, notably baryons (e.g., protons and neutrons) and mesons. In doing so, Glashow had to invent a new property for quarks, which are the fundamental particles that constitute baryons and mesons. This new property, which Glashow called “charm,” provided a valuable extension of the theory of quarks.