questions: - What is the status of the computation of the isgur-wise function F(w) for the B->Dlnu decay, for w far of the kinematics limit w=1? We are aware of recent progress in quenched calculations, what about unquenched? - Is there any attempt to reduce the theoretical uncertainty on the F*(1) (~4%) for the B->D*lnu? - Which are the progress on the B->D**lnu decays, in particular regarding the 1/2 vs 3/2 puzzle for D** states? - Several theoretical arguments would suggest an dominance of the excited J=3/2 D** states vs the J=1/2 states. How the theory would be able to accomodate a scenario with the opposite trend? - Does lattice theory obey the constraints derived from dispersion relations and/or sum rules? - Can form-factors of light mesons at large Q2 (~10.6^2) shed any light on validity of calculations (lattice or whatever) in the B-sector? - Dispersion relation (e.g., CLN) and sum rule (Oliver et. al) yield virtual identical w-dependence for ISF (hA1) when value of rhosq (=d\xi/dw) near measured value is used, but differ if rhosq far off. Is there a prediction of rhosq implicit in the consistency of these different approaches? If so can lattice shed any light on the subject?