Hands-on practice
Author: Katarzyna KruszyĆska
Contributors: Amber Malaps, Somayeh Khakpash, Rachel Street
Shapes of Planetary Caustics in various regions of the parameter space
Shapes of Planetary Caustics as a function of projected separation
Gaudi 2021
$$s = \frac{u \pm \sqrt{u^{2} + 4}}{2},$$
where
$$u = \sqrt{u_{0}^{2} + \left(\frac{t_{0}-t_{p}}{t_{E}}\right)^{2}}$$
$$t_{Ep} = \sqrt{(q + \rho^{2})} \times t_{E}, \rho = \frac{t_{*}}{t_{E}}$$
$$u = \sqrt{u_{0}^{2} + \left(\frac{t_{0}-t_{p}}{t_{E}}\right)^{2}}$$
$$s = \frac{u \pm \sqrt{u^{2} + 4}}{2}$$
When ρ > caustic
$$\rho = \frac{t_{*}}{t_{E}}$$
The following images illustrate the light curve features (aka perturbations) corresponding with different source images and caustic structures.
Review these images, then work through the notebooks provided, using the gallery to interpret the light curves in the exercises.
In order to use them, please make sure you have these packages installed in your environment.