Oriented attachment of nanocrystalline subunits is recognized as a common crystallization pathway that is closely related to formation of nanoparticle superlattices, mesocrystals, and other kinetically stabilized structures. Approaching particles have been observed to rotate to achieve coalignment while separated by nanometer-scale solvent layers. Little is known about the forces that drive coalignment, particularly in this "solvent-separated" regime. To obtain a mechanistic understanding of this process, we used atomic-forcemicroscopy-based dynamic force spectroscopy with tips fabricated from oriented mica to measure the adhesion forces between mica (001) surfaces in electrolyte solutions as a function of orientation, temperature, electrolyte type, and electrolyte concentration. The results reveal an ∼60°periodicity as well as a complex dependence on electrolyte concentration and temperature. A continuum model that considers the competition between electrostatic repulsion and van der Waals attraction, augmented by microscopic details that include surface separation, water structure, ion hydration, and charge regulation at the interface, qualitatively reproduces the observed trends and implies that dispersion forces are responsible for establishing coalignment in the solvent-separated state.orientation-dependent interparticle forces | dynamic force spectroscopy | atomic force microscopy | solvent structure | DLVO theory C rystallization by particle attachment (CPA) is a common mechanism by which single crystals form in solutions (1). In contrast to classical growth processes of monomer-by-monomer addition and Ostwald ripening, CPA occurs through assembly of higher-order species ranging from multi-ion complexes (2) and polymeric clusters (3) to fully formed nanocrystals. Among the numerous styles of CPA, none has garnered more attention than oriented attachment (OA) by which crystalline nanoparticles assemble into larger single-crystal structures through attachment on coaligned crystal faces (4, 5). OA often leads to formation of hierarchical structures, such as highly branched nanowires (6), tetrapods (7), and nanoparticle superlattices (8), endowed with unique properties (9) that are inexorably tied to this nonclassical process of crystallization.OA has been inferred for metals (10), semiconductors (11), and insulating oxides (6); it has been directly observed via liquid phase transmission electron microscopy (LP-TEM) (5), and the evolution of particle distributions during OA has been captured with cryogenic TEM (12). OA is highly dependent on solution conditions, including pH, ionic strength, and temperature, and is marked by two important stages. In the first stage, particles approach one another but do not make contact; rather they remain separated by an intervening solvent layer of O(1) nm in thickness (5). This solvent-separated state can occur on such an extensive scale that a kinetically stabilized particle array-sometimes referred to as a mesocrystal-is formed in which particles are crystallographically...