The maximal conserved phase gradient is introduced as an order paramet
er to characterize the transition from phase to defect turbulence in t
he complex Ginzburg-Landau equation. It has a finite value in the phas
e-turbulent regime and decreases to zero when the transition to defect
turbulence is approached. Solutions with a nonzero phase gradient are
studied via a Lyapunov analysis. The, degree of ''chaoticity'' decrea
ses for increasing values of the phase gradient and finally leads to s
table traveling wave solutions. A modified Kuramoto-Sivashinsky equati
on for the phase dynamics is able to reproduce the main features of th
e stable waves and to explain their origin.