In this paper I investigate mean-field effects for a Bose gas harmonically trapped above the quantum transition temperature in the collisionless regime. I point out that these effects can play a role in low dimensional systems. My treatment relies on the Boltzmann equation with the inclusion of the mean-field term. I first discuss the equilibrium state then derive the dispersion relation for collective oscillations (monopole, quadrupole, and dipole modes) in D dimensions.
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