In Fig. (e,bottom), we provide a real-space analysis of the κMP2 and MLS2 correlation energy densities along the orthogonal principal plane between the two formic acid fragments. These quantities represent the correlation contribution to the interaction energy (correlation energy density of the dimer minus the corresponding energy densities of individual fragments), allowing us to see how correlation affects binding and nonbinding regions between the two fragments. The strong overbinding in κMP2 is reflected by intense binding regions (red), whereas MLS2 shows lower intensity binding regions and introduces non-binding areas, resulting in major improvements over κMP2 interaction energies. We observe similar improvements of MLS2 over κMP2 for other dissociation curves of noncovalent systems from the S22x5 dataset 61 (see Fig. in the SI). These results further confirm MLS2's transferability, as it successfully extrapolates from dispersion-bound systems (RG18) to distinctly different noncovalent interactions, such as hydrogen bonds.