Mo’ Better Bounds
One of the novelties (for me, at least), in writing a paper in a well-worn field like precision electroweak measurements, is that a lot of people have a prior stake in the subject. Our recent paper got a flood of very positive comments.
All very gratifying. But, at the end of last week, came one comment which made us realize that our bounds (from forward-scattering dispersion relations) could be considerably strengthened. So we spent most of the intervening week redoing our analysis, and rewriting our paper to incorporate the new, stronger bounds.
Forward scattering produced the bounds Theoretically, this was notable because the shape of the allowed region differed from that predicted by the classical superluminality analysis, which can also be thought of as modified classical propagation resulting from (tree-level) forward scattering off a nontrivial background field.
The new, stronger bounds are Unlike the previous case, the 3rd bound is redundant to the other two. A comparison of the old and new bounds can be seen in the figure below.
Theoretically, you might not find the new bounds all that interesting an improvement over the old ones. But, when you compare them with what might be measured experimentally at the ILC, the new, tighter bounds become somewhat more interesting experimentally.
There’s more work to be done, but one can kinda get a rough idea by comparing our bounds with the following graph from Boos et al. To make the comparison, .
What one would like to show, for instance, is that a measurement which yielded that 90% CL ellipse implies a violation of our bounds …