We analyze the exact perturbative solution of N=2 Born–Infeld theory which is believed to be defined by Ketovʼs equation. This equation can be considered as a truncation of an infinite system of coupled differential equations defining Born–Infeld action with one manifest N=2 and one hidden N=2 supersymmetries. We explicitly demonstrate that infinitely many new structures appear in the higher orders of the perturbative solution to Ketovʼs equation. Thus, the full solution cannot be represented as a function depending on a finite number of its arguments. We propose a mechanism for generating the new structures in the solution and show how it works up to 18-th order. Finally, we discuss two new superfield actions containing an infinite number of terms and sharing some common features with N=2 supersymmetric Born–Infeld action.