Quantum oscillations have played a major role in the history of condensed matter physics-and indeed in physics as a whole. In 1930, Shubnikov and de Haas (SdH) [1] discovered oscillations in the resistance of bismuth as a function of magnetic field, R(B). Because of theoretical work of Landau [2] in the same year, it was soon realized that the oscillations were periodic in 1/B: if a peak in R is observed at B = 1 T and another at B = 0.5 T, then we should see one at B = 0.33 T, B = 0.25 T and so on. This work is famous, but maybe not as much as it should be: it was the first discovery of a macroscopic effect that depends for its existence on the fact that an electron has a phase. The magnetic susceptibility also oscillates. This is the deHaas-van Alphen effect, also a product of the year 1930. The Hall resistance does as well, but in bulk materials the effect is not so big. All of these effects are periodic in 1/B, just like the SdH oscillations. It must be so, since all of these quantities depend on the density of electron states at the Fermi energy ρ(E F), and it is this underlying physical quantity that is periodic in 1/B. These discoveries were dramatic in that they were a beautiful demonstration of quantum mechanics in bulk materials. The observation of Onsager [3] in 1952 that the period in (1/B) is inversely proportional to the extremal cross section of the Fermi surface meant that SdH and dHvA effects could be used for the measurement of band structure,