Constructing self-referential instances for the clique problem
Jiaqi Li, Shuli Hu, Xianxian Li, Minghao Yin
TL;DR
This work addresses the inherent hardness of the clique problem by proving a precise phase transition for the existence of a $k$-clique in $G(n,m)$ and constructing self-referential, degree-preserving graph instances at the transition. The authors combine first- and second-moment analyses to locate the threshold at $m = rac{n(n-1)}{2} obreak\cdot n^{-rac{2}{k-1}}$, showing whp nonexistence below and whp existence above it. They then build a class of graphs sharing $|V|$, $|E|$, and degree sequence that can be transformed between having and lacking a $k$-clique via symmetric operations, with the transformed instance unlikely to retain a clique, thereby forcing exhaustive search in the critical regime. The results illuminate why solution-space independence necessitates exhaustive verification at the phase transition and suggest that this self-referential construction approach can extend to other combinatorial problems.
Abstract
In this paper, we propose constructing self-referential instances to reveal the inherent algorithmic hardness of the clique problem. First, we prove the existence of a phase transition phenomenon for the clique problem in the Erdős--Rényi random graph model and derive an exact location for the transition point. Subsequently, at the transition point, we construct a family of graphs. In this family, each graph shares the same number of vertices, number of edges, and degree sequence, yet both instances containing a $k$-clique and instances without any $k$-clique are included. These two states can be transformed into each other through a symmetric transformation that preserves the degree of every vertex. This property explains why exhaustive search is required in the critical region: an algorithm must search nearly the entire solution space to determine the existence of a solution; otherwise, a counterinstance can be constructed from the original instance using the symmetric transformation. Finally, this paper elaborates on the intrinsic reason for this phenomenon from the independence of the solution space.
