I'm sorry my title is not descriptive; the function I am interested in is too long to put in there. What I am looking at is the roots of the following function: $f(\epsilon) = (\Delta^2-\epsilon^2)(\epsilon^2 - (\Gamma_1+\Gamma_2)^2/4) + \Delta^2 \Gamma_1 \Gamma_2 \sin^2(\phi/2) + (\Gamma_1+\Gamma_2)\,\epsilon^2\,\sqrt{\Delta^2-\epsilon^2}$
Here all parameters are real numbers.
Now, this function is readily evaluated with numerical methods, but I would like to know if there is some analytics we can do to end up with expressions for how things scale.
Specifically, I am interested in the limiting behavior of $\epsilon$ (for which $f(\epsilon) = 0$) around $\phi = \pi$, and its scaling with $\delta = \vert{\Gamma_1-\Gamma_2}\vert$. Indeed, one finds that for $\Gamma_1 = \Gamma_2$, $\epsilon = 0$ at $\phi = \pi$. I'd like to know how $\epsilon$ approaches 0 as $\delta$ goes to 0. Is that something that is possible analytically?
Some assumptions we can tack on, if needed, and it probably is, is that either $\Delta \gg \max{(\Gamma_1,\Gamma_2)}$, or $\min{(\Gamma_1,\Gamma_2) \gg \Delta}$, where the former has my preference as its closer to the situation I want to investigate, but the latter also has some value.
For context, the equation comes from Resonant Josephson Current through a Quantum Dot by Beenakker and van Houten from 1992 and describes the energy-phase relationship of a bound state in the system.