Maybe this is trivial, but the action of a conformally coupled scalar is $$ S = \frac{1}{2} \int d^Dx \sqrt{g} (g^{ab} \partial_a \phi \partial_b \phi + \xi R \phi^2),$$ where $\xi = (D-1)/4D$. Does this imply that... ... a theory of conformally coupled scalars is always massive (i.e., there exi...