Fig. 18

The distributions of the signature distances \(d_{\text {sn}}(s,\Omega )\) and \(d_{\text {sn}}(s,\Omega _{\text {probe}})\) between the target s and two types of Boltzmann ensembles. LHS utilizes unrestricted samples \(\Omega \) of structures, and RHS uses samples \(\Omega _{\text {probe}}\) incorporating probing data simulated from the signature of the target structure s