Dispersive chaos is a dynamical state that consists of the repeated, irregu
lar growth and abrupt decay of spatially localized bursts of traveling wave
s. This state can be observed just above onset in convection in binary flui
ds at small, negative separation ratio psi in a long, quasi-one-dimensional
geometry. We describe experiments in which this erratic behavior is suppre
ssed by applying as feedback a spatially varying Rayleigh-number profile co
mputed from the measured convection pattern. With the appropriate feedback
algorithm, an initial state consisting of unidirectional traveling waves of
spatially uniform amplitude and wave number can be maintained in a steady
state over a large fraction of the unstable branch of the subcritical bifur
cation to convection. This allows us to measure the nonlinear coefficients
of the corresponding quintic complex Ginzburg-Landau equation.