Hoi Alessio, very nice talk! Here are just a few nit-picking comments: p2: "model dep." not due to mb, a parameters, but rather due to shape function parametrization. The parameters per se are HQET "theory" parameters, not a model. But the specific form of SF parametrization in deFazio/Neubert is a model. Which is THE reason why we want to avoid a dependency on the SF. p4: I would flip the x-y axes for the "correlation" plot, then it's the same as other people use, e.g. in the canonical plot of Bauer/Ligeti (Fig 1 of ph/0107074). I think in general this is called a "Dalitz" plot, not a "correlation" plot. p5: I do not think that we need to go as high as 10 GeV2. In fact, IF we want to put out a result as soon as possible with minimal changes, I would argue that the q2 cut should be relatively low, with higher mX cuts than what we have done so far. See e.g. table I in ph/0107074. Why 10Gev2? I have to admit that I have not yet clicked through all the links in your webpage, I don't know whether you have done this. Ed has produced scans in the (mX, Q2) plane. p6: I think that this should be a 2-d scan in (mX,q2), not just a 1-d scan. You must look at different combinations. Not only "sys" reduction, but "sys^2 + theo^2". We will not gain in "sys" probably. p7: Naive question: Why does the efficiency flatten at mX = 1.8GeV? Applying a q2 > 10 GeV2 should leave signal rate to higher mX (both from your plot on page 4 and from ph/0107074). Again, I think that it should be a 2-d scan of the error not only vs. q2, but in the full (q2,mX) plane. p8: By now I think I was confusd and what you call "sys" is actually "theo"; OK... p9: I would propose that we very seriously consider switching to the non-resonant as "default" signal MC. Of course we need to understand the behavior of the error on the hybrid MC. p10 I would feel (very) uncomfortable to extract mb from a spectrum that shows a disagreement between the model and data as shown in the bottom left two plots. Before we do that we should be sure that e.g. changing neutrals selection and tracking has a very small effect on this. There is work ongoing by Jonathan Coleman which we should look at. I consider this one of the more important improvements (on a time scale longer than this summer) for the incl b2u analyses. p12 Again, I personally would not claim that we can extract mb from the mX distribution to 80MeV. p18 "1." I would maybe say that we need to understand the hybrid MC "For this summer 2." I would say we need to validate the spectra other than mX given from the fit. That's all for now. Cheers, --U.