Self-assembled molecular helices are ubiquitous in nature and can be found in many biologically important macromolecules. It is therefore not surprising that chemists have made significant efforts to introduce helicity in many artificial systems. [1] The inherent chirality present in such spiral structures is generally associated with enantioselectivity [2] or interesting optoelectronic properties. [3] Theoretical [4] and experimental [5] studies have indicated that helical supramolecular networks can affect chiral ordering in crystal lattices.Molecular helicity can be programmed by judicious selection of elements that are encoded with structural and conformational information designed to enforce intramolecular self-organization in a spiral arrangement. Examples such as helicenes, [6] poly(m-phenylene), [7] polyheterocyclic strands, [8] m-phenylacetylene oligomers, [9] b-peptides, [10] polyisocyanates, [11] and oligoarylamides [12] elegantly illustrate this concept. The generation of supramolecular helices requires an additional design element, namely, a reliable noncovalent motif that can provide the desired connectivity of the building blocks in a predictable manner. Hydrogen bonds, [13] metal coordination, [14] and p ± p stacking interactions [15] are often utilized in this regard. These design strategies, however, are generally limited to one dimension, coinciding with the helix direction, while the assembly and structure along the remaining two crystal dimensions are difficult to control. The rational construction of new materials with tailored functions and properties, however, requires control of crystal architecture in all three dimensions. Here we report the formation of hydrogen-bonded helices with predictable three-dimensional (3D) organization in the solid state. This study represents a key first step towards the rational design of crystalline, hydrogen-bonded chiral networks with potential applications in enantioselective separation. [16] We are actively involved in the design of molecular crystals based on the self-assembly of complementary guanidinium and organosulfonate ions, which typically crystallize in a quasihexagonal hydrogen-bonded network (Figure 1 a). [17] These 2D layers can be described as consisting of 1D ribbons along a 1 . The S ¥¥¥ S distance along this axis is nominally identical for all these compounds (7.5 AE 0.2 ä). The ribbons themselves aggregate by hydrogen bonding along the orthogonal direction b 1 . The magnitude of b 1 can vary significantly (7.3 ± 13 ä) as a result of puckering of the sheet about the hydrogen bonds that connect the ribbons. [24] CID was achieved by isolation of the ion of interest in the ion trap, then applying 0.1 ± 1.0 V AC resonance excitation at the secular frequency of the ion and allowing it to collide with helium gas.[25] M.