Particle physics evolved from its roots in cosmic-ray and nuclear physics when scientists realized that there are more fundamental constituents of matter than just protons and neutrons. Over many years, increasingly sophisticated experiments provided the information needed to develop the underlying theoretical concepts. Although the primary experimental results on which the emerging standard model (SM) was built were published elsewhere, Reviews of Modern Physics has been pivotal in putting them into context.
At CERN’s Large Hadron Collider, a Higgs boson and a W boson are produced. In this reconstruction, the Higgs decays into its most likely state of two bottom quarks that then create jets of hadrons (blue cones). The W boson decays into a muon (red line) and a neutrino (white dotted line). (Courtesy of CERN.)
At CERN’s Large Hadron Collider, a Higgs boson and a W boson are produced. In this reconstruction, the Higgs decays into its most likely state of two bottom quarks that then create jets of hadrons (blue cones). The W boson decays into a muon (red line) and a neutrino (white dotted line). (Courtesy of CERN.)
Broken symmetries in the weak interaction
Symmetries have been central to the development of the SM. The demonstration that weak-interaction decays are not invariant under spatial reflection1 showed that they violate parity symmetry. More surprisingly, the combined operation of matter–antimatter interchange (C) and spatial reflection (P) was found to be violated in neutral kaon decays2 at the 0.1% level. There was no explanation for that effect until it was recognized in 1973 that a model with three generations of quark pairs would also allow for CP violation in decays of neutral B mesons,2 which was observed in 2001. The similarity between the weak and electromagnetic interactions, and the observed short range and parity violation of the weak interaction, implied the existence of massive, spin-1, force-carrying bosons with both vector and axial-vector components. The W+, W−, and Z0 bosons discovered3 at the CERN proton–antiproton collider in 1983 verified that prediction.
The nonconservation of probability predicted in processes involving those bosons at high energy was ultimately “repaired” by the Higgs mechanism responsible for spontaneous symmetry breaking of a unified electromagnetic and weak interaction. The symmetry breaking provided the raison d’être for the observed massless photon and massive W+, W−, and Z0 bosons and for the spin-0 Higgs boson discovered4 in 2012.
The observation that neutrinos produced from the decay of a pion into a muon and a neutrino subsequently interact to produce muons but not electrons5 was a surprise and meant that these neutrinos differ from those produced from nuclear beta decays. Another great surprise was the realization that neutrinos from the Sun6 and from particle decays in atmospheric cosmic-ray showers7 transform from one type to another. Those findings—and the discovery8 of the τ, the third charged lepton—revealed that there are three generations of charged lepton and neutrino pairs and that at least two of the neutrinos have nonzero mass.
Revealing the strong interaction
The notion that mesons and baryons are composed of quarks was bolstered experimentally9 in the early 1970s. Three quark flavors—up, down, and strange—were sufficient to explain the patterns of the known hadrons until 1974, when experiments at Brookhaven and SLAC revealed a new meson carrying a fourth quark flavor, charm.10 Subsequent experiments at Fermilab found the even heavier bottom and top quarks11 and thus established that, just as for the leptons, there are three generations of quark pairs.
The SM theory of the strong interactions was built on such observations as highly inelastic scattering of electrons and neutrinos from nucleons.12 The scattering first revealed the nucleon’s point-like constituents, thus supporting the quark picture, and subsequently showed the characteristic momentum-transfer dependence of their coupling to gluons—the mediators of the strong force—that is at the heart of quantum chromodynamics (QCD). Experiments verified calculations of many hadronic cross sections at high energy13 and thereby established the validity of QCD as the theory of strong interactions.
Although the SM has by now been verified by thousands of measurements, it remains a mysterious success. For instance, it contains 26 ad hoc parameters—masses, mixing angles, couplings, and so on—that, if modified, would lead to an unrecognizably changed universe.14 And although the SM edifice is well founded, it is manifestly incomplete!
Tools and instruments
The pioneering measurements discussed here would not have been possible without the increasing sophistication and power of experimental tools.15 Accelerators evolved from tabletop cyclotrons to colliders tens of kilometers in circumference. Instruments that measure particle reactions grew in size, complexity, and precision—from early cloud chambers to huge multielement electronic detectors. The revolution in computing greatly expanded the reach of experiments. And newly developed technologies have found applications in medicine, industry, national security, and other sciences.16
The rapidly expanding base of knowledge about the SM needed an evolving compendium of numerical information about the properties of the myriad particles and their interactions. Reviews of Modern Physics published frequent updates of such information, beginning with a 1964 article on particle properties.17 In fact, the journal has served as an archive of the fundamental constants of our science since its first article, “Probable values of the general physical constants,” was published.18
The rest of the Reviews of Modern Physics 90th anniversary articles can be found in the special feature’s introduction by Randall Kamien.
References
Paul Grannis is a research professor of physics at Stony Brook University in New York. Vera Lüth is a professor emerita at Stanford University in California.
