One of the fundamental open problems in the area of distributed graph algorithms is the question of whether randomization is needed for efficient symmetry breaking. While there are fast, poly log n-time randomized distributed algorithms for all of the classic symmetry breaking problems, for many of them, the best deterministic algorithms are almost exponentially slower. The following basic local splitting problem, which is known as the weak splitting problem takes a central role in this context: Each node of a graph G = (V, E) has to be colored red or blue such that each node of sufficiently large degree has at least one node of each color among its neighbors. Ghaffari, Kuhn, and Maus [STOC '17] showed that this seemingly simple problem is complete w.r.t. the above fundamental open question in the following sense: If there is an efficient poly log n-time determinstic distributed algorithm for weak splitting, then there is such an algorithm for all locally checkable graph problems for which an efficient randomized algorithm exists. In this paper, we investigate the distributed complexity of weak splitting and some closely related problems and we in particular obtain the following results:• We obtain efficient algorithms for special cases of weak splitting, where the graph is nearly regular. In particular, we show that if δ and ∆ are the minimum and maximum degrees of G and if δ = Ω(log n), weak splitting can be solved deterministically in time O ∆ δ · poly(log n) . Further, if δ = Ω(log log n) and ∆ ≤ 2 εδ , there is a randomized algorithm with time complexity O ∆ δ · poly(log log n) . • We prove that the following two related problems are also complete in the same sense:(I) Color the nodes of a graph with C ≤ poly log n colors such that each node with a sufficiently large polylogarithmic degree has at least 2 log n colors among its neighbors, and (II) Color the nodes with a large constant number of colors so that for each node of a sufficiently large at least logarithmic degree d(v), the number of neighbors of each color is at most (1 − ε)d(v) for some constant ε > 0.