Abstract
We study the effect of steepness in smooth phase changes in the laser that drives an optomechanical system in the red-detuned, linearized regime. These phase changes take the semi-classical component out of its steady state. Steeper phase changes produce larger amplitudes for the fast oscillations in the mean fields. In contrast, sufficiently slow phase changes keep the system close to its steady state and allow the implementation of a phase driving scheme designed to minimize the variation of the quantum fluctuation mean excitation values.
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