Hi all, I started investigating the possibility of using the Q2 variable. I just looked at possible advantages in the statistical error (no theoretical error was taken into account) adding a cut on Q2. First, these are the Q2 vs Mx plots for the signal and the background: http://www.slac.stanford.edu/~daniele/vub/Q2vsMx_vub.ps signal http://www.slac.stanford.edu/~daniele/vub/Q2vsMx_vcb.ps vcb bkg Then I studied the dependence of the statistical significance as a function of a cut on Q2 (for different cuts on Mx). This is the result for Mx<1.55GeV. http://www.slac.stanford.edu/~daniele/vub/mx155.ps top left: S/sqrt(S+B) vs cut on Q2 (S=vub events, B=vcb events both for Mx < Mxcut) top right: S vs cut on Q2 bottom left: S vs cut on Q2 Similar plots for different Mx cuts. As you see, no gain comes from an additional cut on Q2 (as far as the statistical error is concerned). BTW a study of the result as a function of this cut seems to be feasible. The MC statistics used corresponds to ~200 fb-1 (with BR(b->ulnu) = 1.3 * 10-3). With the number of signal events we will have in 80fb-1 (>200) we could perform plots similar to the ones I showed above. It should be very interesting to check the stability of the result as a function of the Q2 cut (since theorists think that the best theoretical error should be obtained with a combined cut). Daniele