  We investigate the possibilities of distinguishing the mean-field and
fluctuation effects on the critical temperature of a trapped Bose gas with
repulsive interatomic interactions. Since in a direct measurement of the
critical temperature as a function of the number of trapped atoms these effects
are small compared to the ideal gas results, we propose to observe
Bose-Einstein condensation by adiabatically ramping down the trapping
frequency. Moreover, analyzing this adiabatic cooling scheme, we show that
fluctuation effects can lead to the formation of a Bose condensate at
frequencies which are much larger than those predicted by the mean-field
theory.
