The metal-insulator transition (MTT) observed in two-dimensional (2D) syste
ms is apparently contradictory to the well-known scaling theory of localiza
tion. By investigating the conductance of disordered one-dimensional system
s with a finite phase coherence length, we show that by changing the phase-
coherence length or the localization length, it is possible to observe the
transition from insulator-like behavior to metal-like behavior, and the tra
nsition is a crossover between the quantum and classical regimes. The resem
blance between our calculated results and the experimental findings of 2D M
IT suggests that the observed metallic phase could be the result of a finit
e dephasing rate.