interaction, ultimately determine the final deposition and morphology of patterns. [4][5][6][7][8][9] Various approaches have been explored to modify these interactions in order to control the contact line dynamics and/or to induce Marangoni flow driven by the surface tension gradient on the air-droplet interface, including tuning substrate wettability, [10,11] application of surfactant additives and cosolvent systems to the droplet, [12,13] vapor absorption of low-surface tension solvents to the droplet, [14] etc. In these techniques, the colloidal particles are carried back to the center of the droplet either by the depinned contact line or by Marangoni flow to suppress the coffeering effect. In addition, stronger interactions between colloidal particles and substrates, e.g., electrostatic and van der Waals interactions, [15] and increased adhesion through substrate treatment, [16] etc. also facilitate a uniform deposition. Recently, attempts have been made to push the colloidal particles onto the droplet surface to facilitate the particle selfassembly at the air-droplet interface. [17] Boley et al. have employed a cosolvent system for the colloidal particles. [18] During evaporation, the colloidal particles which are well-dispersed in the solvent with a higher vapor pressure are carried to the droplet surface due to faster evaporation of this solvent component. Li et al. have accelerated the solvent evaporation rate to trap the particles at the droplet interface by elevating the environment temperature. [19] At a high environment temperature, the air-droplet interface shrinkage rate exceeds the particle diffusion rate such that the colloidal particles are captured by the descending surface, producing a particle jam which prevents them from being transported to the droplet edge. The charges of surfactant-decorated particles have also been tuned to become nearly neutral, [20,21] which promotes particle trapping at the air-droplet interface to render a homogeneous deposition.In this work, we employ a dual-droplet configuration to transform the Langmuir-Blodgett (LB) concept to the picoliter droplets generated by inkjet printing. Deposition of monolayer nanoparticle films is achieved by a consecutive dual-droplet printing of a supporting droplet and a wetting droplet (Figure 1). The supporting droplet acts as the LB trough, and the wetting droplet contains colloidal nanoparticles. The colloidal particles spread over the supporting droplet surface and assemble at the interface as the solvent dries to produce a uniform, nearlyThe well-known coffee-ring effect causes colloidal particles to convectively transport toward the contact line of an inkjet droplet leading to a nonuniform deposition of the colloidal particles. In this work, the self-assembly of colloidal particles in a dual-droplet inkjet printing configuration to produce a nearly monolayer closely packed deposition of colloidal particles that exhibits a colorful reflection are demonstrated. By controlling the ink surface tensions and jetting parameters, the ...