Understanding how a stereogenic center influences conformations at the molecular scale and organization at the supramolecular level is an elusive and intriguing challenge in a number of scientific disciplines. [1] A very interesting challenge is to prepare self-assembling systems and to study how the chiral nature of the component compounds in combination with the self-assembly process affects the ordering in two and three dimensions. In both two-and threedimensional (2D and 3D, respectively) systems, pure enantiomers form enantiomorphous structures.But what happens when equimolar mixtures of enantiomers are crystallized or are physisorbed at a surface? Will the racemate resolve spontaneously into a racemic conglomerate, or will both enantiomers co-crystallize or co-adsorb forming racemic 3D or 2D crystals? In 3D (liquid) crystals, conglomerate formation is the exception [2,3] rather than the rule. In 2D monolayers at the air/water interface, both the controlled separation of enantiomers and racemate formation have been reported from grazing incidence X-ray diffraction studies. [4,5] In 2D monolayers on solid supports, modern tools such as atomic-force microscopy (AFM) [6] and scanning tunneling microscopy (STM) provide compelling evidence for spontaneous segregation. [7] The use of STM is especially appealing for the visualization of (sub)monolayer structures, since it can reveal with near-atomic resolution the ordering in two dimensions. [8] The technique has shown that both chiral [9±11] and achiral [12,13] molecules self-assemble into chiral arrays, the former enantiospecifically and the latter as 2D conglomerates. Experimental data available so far suggest a spontaneous resolution, [9a, 10, 11a±d] although one report has noted differences in the way molecules discriminate through their chirality depending upon their absorption site. [14] The compounds we have targeted to address these questions are the achiral formamide 1 and the chiral formamide 2. [15] Here we report the X-ray crystal structure and STM imaging of the self-assembled monolayers of the enantiopure and racemic 2, as well as the STM data for 1, and compare the expression of molecular chirality in two and three dimensions.The X-ray crystal structure [16,17] of the enantiopure compound (R)-2 ( Figure 1) has a unit cell which contains molecules with four different conformations, all of which form chains (in which the molecules are linked through NÀH´´´OC and other weaker hydrogen bonds) that unite head-to-head through CÀH´´´OC hydrogen bonds between formyl groups to generate supramolecular tapes. There are Figure 1. Views of the two hydrogen-bonded tapes formed by the four conformational diastereomers of (R)-2 in its crystals. Intrachain NÀH´´´O distances: 2.072 and 1.940 ; angles: 167.4 and 157.98; N´´´O distances: 2.864 and 2.857 ; interchain CO´´´HÀC distances: 2.685, 2.693, 2.675, and 2.