An Algorithm for Computing Lipschitz Inner Functions in Kolmogorov's Superposition Theorem

Kolmogorov famously proved that multivariate continuous functions can be represented as a superposition of a small number of univariate continuous functions, $$ f(x_1,\dots,x_n) = \sum_{q=0}^{2n+1} \chi^q \left( \sum_{p=1}^n \psi^{pq}(x_p) \right).$$ Fridman \cite{fridman} posed the best smoothness bound for the functions $\psi^{pq}$, that such functions can be constructed to be Lipschitz continuous with constant 1. Previous algorithms to describe these inner functions have only been H\"older continuous, such as those proposed by K\"oppen and Braun and Griebel. This is problematic, as pointed out by Griebel, in that non-smooth functions have very high storage/evaluation complexity, and this makes Kolmogorov's representation (KR) impractical using the standard definition of the inner functions. To date, no one has presented a method to compute a Lipschitz continuous inner function. In this paper, we revisit Kolmogorov's theorem along with Fridman's result. We examine a simple Lipschitz function which appear to satisfy the necessary criteria for Kolmogorov's representation, but fails in the limit. We then present a full solution to the problem, including an algorithm that computes such a Lipschitz function.