Fission product yield is primarily a function of two things:
1. The type of fissile nuclide
2. The energetics of the compound nucleus post-absorption and pre-fission.
As far as I know, both the APWR and PBMR will still use U-235 as its primary fissile nuclide. They may be in unique geometries or forms (e.g. PBMR's TRISO fuel kernels), but in general, for commercial applications, U-235 enrichment would still be very low. Consequently, the distribution of fissile materials, including the transuranic elements produced during operation, will probably be the same as current LWR's.
For U-235, the fission yield curve is the double hump curve with maximum frequencies at around atomic masses of 90 and 140. The depth of the valley in between depends on the stored energy of the compound nucleus. In general, fissions induced by thermal neutrons demonstrate a very shallow valley, whereas fast neutrons will render the double peaks less distinguishable. APWR and PBMR are all thermal reactors.
So, unless future designs dictate a more exotic fuel (e.g. MOX, actinide fuel) or a faster neutron spectrum, the double hump fission yield is a good approximation.
You can find the curve on wiki or any introductory nuclear engineering textbook.