  The scaling theory of the transitions between plateaus of the Hall
conductivity in the integer Quantum Hall effect is reviewed. In the model of
two-dimensional noninteracting electrons in strong magnetic fields the
transitions are disorder-induced localization-delocalization transitions. While
experimental and analytical approaches are surveyed, the main emphasis is on
numerical studies, which successfully describe the experiments. The theoretical
models for disordered systems are described in detail. An overview of the
finite-size scaling theory and its relation to Anderson localization is given.
The field-theoretical approach to the localization problem is outlined.
Numerical methods for the calculation of scaling quantities, in particular the
localization length, are detailed. The properties of local observables at the
localization-delocalization transition are discussed in terms of multifractal
measures. Finally, the results of extensive numerical investigations are
compared with experimental findings.
