Nematic liquid crystals (LCs) are anisotropic elastic fluids and their molecular orientation can be controlled by surfaces and external electric/magnetic fields. These properties make them highly attractive for fabrication of tunable devices such as displays, [1] spatial light modulators, [2] dynamic lenses [3] and artificial muscles, [4] and for the manipulation of guest materials as a tunable anisotropic host. [5][6][7][8] Here, we report a novel method for LC alignment based on micrometer-scale photolithographic patterning of a self-assembled monolayer (SAM) coated onto an indium tin oxide (ITO) surface. We use closed vertically aligned LC-boundary walls, induced by the SAM surfaces, to control planar alignment of LCs on the isotropic ITO surfaces. This simple approach not only presents a new concept of planar LC alignment, which, so far, has been achieved only by nanometer-scale anisotropic surfaces, but also provides a compartmentalization of those planar-aligned LC domains. This compartmentalization allows the planar domains to be switched independently by vertical electrical fields without the dynamic LC crosstalk (molecular orientation interference between neighboring switching LC domains), a serious problem that is known to degrade current LC devices. [9][10][11] Due to the symmetry of the SAM patterns, our compartmentalized LC cells show multistable states that are tunable by an in-plane bias. The described method, exploiting mature lithography techniques, is highly reliable and cost effective, and it opens new routes for the design and fabrication of multistable LC devices, switchable viewing angle displays, and tunable structures of guest materials within a LC host.It is well known that vertical alignment of LCs can be induced by long-alkyl-chain-terminated surfaces, [1] but achieving reliable and cost-effective planar alignment remains a challenge. [12] Existing alignment methods, such as mechanical rubbing, photoalignment, and ion-beam bombardment, all rely on nanometer-scale topological or molecular/atomic anisotropy of the alignment surfaces, properties that are difficult to control uniformly on a macroscopic scale. [12][13][14][15][16] Alignment with micropatterned isotropic surfaces, consisting of stripes of alternating random planar-and vertical-aligning materials, has been suggested as a more reliable and cost-effective technique. [13,17] The LC alignment with those stripe patterns suffers, however, from random defects [13,17] due to the finite elastic correlation length of LCs and the tilt degeneracy within the planar stripes. To solve these problems, it has been suggested to use oblique illumination in combination with photoactive SAMs, [13] yet this approach relies again on molecular-level anisotropy of the surfaces.We use patterned surfaces with random planar-aligning squares embedded in a vertical-aligning surface background. The closed vertically aligned LC boundaries induce well-defined planar LC alignment on the random planar squares. A macroscopic in-plane bias, such as a directional ...