I have a question pertaining specifically to a one-matrix model with a multi-cut solution. The standard procedure is to take a polynomial superpotential W(x). In the classical limit (analogous to ℏ=0), all of the eigenvalues are sitting precisely at the extrema of W. As you turn some sort of coupling on, and pass to the large-N 't Hooft limit (the matrices are N×N), the eigenvalues "repel" each other and spread out to form "branch cuts."
I had been assuming that this spreading out from the extrema of W happens symmetrically, but perhaps they won't spread symmetrically if the eigenvalues from the other cuts can repel them? To make my question more concrete, imagine just two extrema of W at ±1 on the real axis. Let's assume the cuts will spread out also on the real axis. Will each cut emerge symmetrically from ±1? Or will they actually spread more on the "outside" since the eigenvalues might repel each other more on the "inside"?
I haven't seen this discussed in the matrix model literature so I was hoping perhaps someone had some insight!
This post imported from StackExchange Physics at 2016-06-26 09:55 (UTC), posted by SE-user spietro