Alternatively, adding 25% exact exchange (to obtain the SCAN0 functional ) results in convergent behavior for MBE(n) as shown in Fig. . This was not the case when SG-2 was used. Instead, SCAN0-MBE(5) errors for this same set of F -(H 2 O) 15 clusters, computed using the SG-2 grid, span a range of almost 250 kcal/mol and lack the telltale alternating signs of SIE-dominated errors. Nevertheless, oscillations in SCAN0-MBE(n) errors obtain using the EML(99,590) grid remain larger than the corresponding HF-MBE(n) values, as shown in Fig. . We attribute this to residual delocalization error in SCAN0, since the smaller HF-MBE(5) errors should provide an estimate of MBE(n) errors due to finite-basis effects (specifically, mismatch between subsystem and supersystem BSSE), and the SCAN0-MBE (5) errors are larger than any such effects.