The phase diagram of the integer quantum Hall effect is numerically determi
ned in the tight-binding model, which can account for overall features of r
ecently obtained experimental phase diagram with direct transitions from hi
gh plateau states to the insulator. In particular, the quantum Hall plateau
s are terminated by two distinct insulating regimes, characterized by the H
all resistance with classic and quantized values, respectively, which is al
so in good agreement with experiments. The physical origin of this peculiar
phase diagram is discussed.