Turbulence arising from the phase instability of planewaves in the com
plex Ginzburg-Landau equation is studied by means of numerical simulat
ions of two-dimensional domains of linear size L ranging from 80 to 51
20. It is shown that, although phase turbulence can be considered as s
ustained and statistically stationary in a finite region of parameter
space for systems of finite size studied over a limited time period, i
t is likely to break down towards amplitude turbulence at the infinite
-size infinite-time ''thermodynamic limit.'' As long as it persists, h
owever, the statistical properties of phase turbulence are well descri
bed within the framework of fluctuating interfaces. Parameters of an e
ffective Kardar-Parisi-Zhang equation governing the large-scale phase
fluctuations are evaluated. The logarithmic behavior predicted for the
linear regime in two dimensions is observed. The crossover to the non
trivial scaling regime is estimated to take place at L several orders
of magnitude larger than the largest size considered here.