Fig. 8: Dissimilarity results for the Shastry-Sutherland model.
From: Certification of quantum states with hidden structure of their bitstrings
Dissimilarity of the ground and the first excited states (with zero total spin) of the Shastry-Sutherland model as a function of the inter-dimer coupling in the σz (a) and the random (b) bases. The inset in panel (a) shows how spins are grouped to obtain flattened bitstrings. c Comparison of the partial dissimilarity profiles obtained for the singlet (J2 = 0) and the Néel (J2 = 1) states in the σz basis.
