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Fig. 14.10 Specific heat in the Bragg-William'

A graph of C1 is shown in Fig. 14.10. Above the critical temperature the specitl\. heat vanishes. This is a consequence of the fact that both the long-range and the.' short-range order vanish in that region in the present approximation. We now tum to the lattice gas. The equation of state for the lattice gas in the.' Bragg-Williams approximation can be immediately obtained through the use l1;' the table of correspondence in Section 14.2:

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Density of state of an electron in a magnetic a pure metal, a series of delta functions mark the positions of the Landau levels. (b) In the presence of impUrities, the Landau levels broaden to bands (shaded region). Localized electrons states fill the gap between Landau bands. EF denotes the Fermi level.

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If the total number of electrons is fixed, then changing the magnetic field will change the filling fraction. A filled level will either become underfilled, or it will spill electrons over to a higher level. In either case, the previous analysis breaks down. However, in a physical sample there are always impurities that trap electrons into localized states. It is the presence of impurities that give rise to the stability of the effect, as shown by the plateau in the data. In Fig. 11.15 we show the density of states in a pure sample as compared with one with impurities. In a pure sample we have a series of 8 functions at the Landau levels, while in the presence of impurities each Landau level is broadened to a band, shown shaded in Fig. 11.15. At low impurity densities these bands do not overlap. The important point is that between the Landau bands the density of states is not zero, as would be the case for a pure sample, but is filled by contributions from localized states. The Fermi level can lie in a continuum between Landau bands, and it can shift in response to a change in the occupancy of the filled Landau band, so that the band beneath it remains filled. Thus, for a certain range of the external magnetic field the lowest Landau band remains completely filled, and our argument applies. The fractional effects are more intriguing. What accounts for the stability of the electron film when the Landau level is only one-third full The answer must lie in the Coulomb interaction among the electrons, but so far we only have preliminary guesses. *

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