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?