With the use of optical second-harmonic generation from liquid-crystal (LC) monolayers adsorbed on rubbed polymer surfaces, a close correlation between the rubbing-induced azimuthal orientational distribution of the LC monolayers and the resulting LC bulk pretilt angle has been observed. A simple model based on epitaxial growth of the bulk LC on top of the first LC monolayer is proposed to explain this correlation. PACS number(s): 61.30.v, 42.65. Ky, 68.35.8s Understanding the physical mechanisms involved in both surface and bulk liquid-crystal (LC) alignment is not only of fundamental interest but also finds its application in numerous electro-optic LC devices. Realization of a large-area monodomain LC layer sandwiched between two glass plates is a prerequisite for optimal performance of these devices. Homogeneous planar alignment (i.e. , parallel to the surface along some easy axis) of a LC layer can be achieved in several ways [1]. The most widely used technique is the rubbing of polymer-coated glass substrates. In order to optimize the performance of the LC device, this planar alignment should be accompanied by a nonzero so-called pretilt (8~), defined as the angle between the average molecular orientation in the bulk (the director) and the surface. Experimental realization and theoretical modeling of (high) pretilt angles with the use of rubbed polymer films has been reported frequently [2-5]. However, the generation of the pretilt on various substrates is not yet understood. Based on a theoretical model developed by Okano [6], Sugiyama et al. recently proposed a model for pretilted nematic LC layers on rubbed polyimide (PI) layers containing alkyl branches [5]. They correlated the polar 8~t o the azimuthal torsional surface coupling strength induced by the interaction of the bulk LC with the aligned alkyl branches at the surface.As a result of the pioneering work of Shen and coworkers on the use of optical second-harmonic generation (SHG) for the study of molecular orientations, the technique recently has been exploited as a surface analytical tool to investigate the LC-interface alignment [7][8][9][10][11][12][13][14]. No direct correlation has been observed between the polar angle of the first LC monolayer adsorbed on surfactantcoated glass substrates and the bulk pretilt [8,9]. Additionally it was shown that at the LC-PI interface a polar ordered LC monolayer exists, with an anisotropic azimuthal distribution, preferentially along the rubbing direction, even at temperatures well above the bulk nematicisotropic transition temperature [10,11]. It was also shown that both the LC monolayer and the LC director in the bulk are then aligned via short-range intermolecular interactions as opposed to long-range elastic interactions [10][11][12]. Combining these experimental results one con-eludes that the picture of a bulk LC, directly interacting with a flat polymer surface, with some distribution of aligned alkyl branches on top of it, seems no longer justified [5]. Instead, we have to consider the interaction o...