I quite liked Dave Woody's suggestion - which is in Bryans list (see below). I think it gives us the quantitative information we want. However I would slightly modify it to make the axes more intiative as I describe below. > > 4. Dave Woody has made a suggestion: > > What about doing a simple linear fit of the (diff-map)^2 to > A + B*(original simulation image)^2 ? > 1/sqrt(B) would be interpreted as the fidelity, i.e., the > errors in the map that are proportional to the image. > 1/sqrt(A) would be the "off-source" dynamic range. > This fit should not be computationally time consuming or > difficult to code. > A similar suggestion was made by Stephane a while ago. I would suggest modifying, so it works with binned data rather than a scatter plot (so the full dynamic range curve can be displayed for each simulation) and also use slightly more intuatitive axes (i.e rms vales rather than square values). In the modification take bins on the x axis equally spaced in Log I_model (perhaps bins covering a factor of two in model intensity) For a given intensity bin - look at all pixel locations in the ERROR image having a intensity value in the MODEL which lies in the intensity range of the bin - for these pixel locations calculate the rms of the pixels in the ERROR image. Plot the Log of this quantity as the y value. This will produce a plot of Log(rms error) versus Log(I_model). It will be interesting to see the shape of this plot, it should be displayed for each model/array_size/array_type CLEAN simulation. The curves might be charactered by a straight line at large Log I implying a single on-source dynamic range - or more likely the shape will be a curve implying different on-source dynmic range as a function of model intensity - plus it will have a saturation at low Log I from which we can estimate the off-source errors and the off source dynamic range. In any case if sufficinetly close to linear its useful to rms error = B I_model + A. as in Daves original suggestion where now B is the on-source dynmamic range and A the size of off source errors (to be divided by the peak value of the model to get 'off-source' dynamic range as conventionally defined by radio astronomers). If it is very significantly curved then a higher order polynomial can be fitted. Also useful to plot would be Log(rms error/I_mod) vs Log I OR Log(I_Mod/rms error) versus Log(I) to give the dynamic range directly as a function of Log I. John.