A drying droplet on a solid surface (i.e., unbound solution) often leads to the formation of irregular structures, including coffee rings, [ 1 ] fi ngering instabilities, [ 2 ] and polygonal networks, [ 3 ] owing to the capillary fl ow induced by nonuniform evaporation fl ux or temperature-gradient-induced Marangoni convection. Hence, the ability to precisely control the capillary fl ow and convective fl ux in dryingmediated self-assembly to create spatially well-defi ned surface structures has received considerable attention. To date, a few elegant studies have demonstrated intriguing means based on the controlled evaporation in confi ned geometries (i.e., bound solution) to delicately tailor the evaporative self-organization process, thereby yielding highly ordered structures. [4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23] For example, by rationally designing the upper curved surface in curve-on-fl at geometries to accommodate different shapes, a wide range of complex surface patterns with unprecedented regularity were readily produced during the course of solvent evaporation by controlled, repetitive pinning-depinning cycles of the three-phase contact line of the droplet constrained in curve-on-fl at geometries. [ 24 ] Recently, chemically patterned surface- [25][26][27] and stamp-assisted deposition methods [28][29][30][31][32][33][34][35] have been exploited for evaporative self-assembly of nonvolatile solutes (e.g., nanoparticles and biomolecules). The use of patterned surfaces or polydimethylsiloxane (PDMS) stamps minimizes uncontrolled droplet shape and possible structural instabilities that may otherwise result in a lack of control over the local dewetting dynamics, and thus produces highly regular surface structures. In a typical capillary-force-induced micromolding process, a micropatterned PDMS mold is in contact with a lower stationary substrate where an evaporating droplet is trapped, covering the lower hydrophobic surface and fi lling up the space between adjacent PDMS patterns by either one of two capillary motions: the upward capillary rising induced by wetting between the nonpolar solvent and the hydrophobic surface of the PDMS mold, [ 36 , 37 ] or the downward capillary depression induced by dewetting between the polar solvent and the PDMS mold. [ 38 ] The former capillary motion has been extensively studied and proven to be more successful. [ 36 , 37 ] In contrast, the latter (i.e., the polar solvent/hydrophobic PDMS system, which is recognized as edge-transfer lithography [ 38 ] ) has rarely been utilized due to diffi cult control over the dewetting of the solution. The capillary action of the solution constrained in the confi ned geometry can be signifi cantly infl uenced by the shape and curvature of the molds, thereby providing new opportunities for controlling the local dewetting dynamics to form ordered structures. [ 24 ] Herein, we demonstrate a facile route to creating λ -DNA microring arrays via dewetting-induced self-assembly guided by liquid capillary m...