Inducibility constants for the unresolved 3-cube configurations

Determine the inducibility constants for the three non-equivalent configurations \(W_3=\{(0,0,0)\}\), \(W_4=\{(0,0,0),(1,0,0)\}\), and \(W_5=\{(0,0,0),(0,0,1),(0,1,0)\}\) in \(Q_3\), whose best known lower bounds are respectively \(1/2\), \(4/9\), and \(1/3\).

Background

The paper resolves five previously difficult configurations in {0,1}3\{0,1\}^3, denoted by W7,W8,W9,W10,W12W_7,W_8,W_9,W_{10},W_{12}. It then identifies the remaining three non-equivalent 3-dimensional configurations for which the inducibility constant was not known. The authors report that the numerical upper bound for W5W_5 is close to, but does not coincide with, its known lower bound, indicating that resolving these cases may require methods beyond the calculations used in the paper.

References

Thus, there are only three non-equivalent $H\subseteq {0,1}3$ for which we do not know the inducibility constant: W_3 := {(0,0,0)},\quad W_4 := {(0,0,0),\,(1,0,0)}, \quad W_5 := {(0,0,0),\,(0,0,1),\,(0,1,0)}.

Some exact values of the inducibility and statistics constants for hypercubes  (2503.03408 - Bodnár et al., 5 Mar 2025) in Section 1, Introduction