Since their discovery, columnar mesophases have become increasingly important in fundamental research and in practical applications [1,2] due to their peculiar supramolecular architectures that allow one-dimensional charge transport. Although the most studied columnar phases are formed by disc-shaped molecules, it is now recognized that such phases can also be formed by dendrimers, [3,4] main-or side-chain polymers with [5,6] or without [7±9] mesogenic moieties, phasmids, [10,11] and board-shaped molecules. [12] For most applications, the organization of the columnar phase at different spatial scales, as well as its temperature and time stabilities are of primary importance. Indeed, at the local scale the mutual mesogen orientation and intracolumnar ordering directly affects charge migration [13,14] and could possibly be tailored to maximize electron orbital overlap. The electronic and optical properties of the liquid-crystalline (LC) phases also strongly depend on the large-scale structure. In particular, the organization at the mesoscopic scale, ranging from several nanometers to some hundreds of nanometers, must be tailored to control features such as the size and orientation of the LC monodomains. This spatial scale is, however, not easily assessable by conventional techniques [15] as it falls in the gap between the resolution of conventional optical observations and X-ray diffraction. As far as temperature and time stability of the phases are concerned, it is worth noting that the phase diagrams of systems forming LC columnar mesophases are generally complex. This is often not only due to a rich polymorphism of these systems, but also to the heating/cooling irreversibility of phases, i.e., the appearance of monotropic phases. The latter are typically observed on cooling when the phase that is energetically more stable is bypassed because of the slow (re)crystallization kinetics. It is important to note that crystallization of the mesophases was previously studied in some detail for highly ordered smectic phases (G and H) formed by calamitic molecules. [16] Compared to the monotropic nematic and smectic phases formed by polymers, [17,18] the columnar LC monotropic phases have been less extensively studied. [19±22] Two of the first LC molecules displaying monotropic columnar phases were observed by Giroud-Godquin et al. [23] (in metallomesogens) and by Billard et al. [24] (in rufigallol hexa-n-octanoate). In the first case, the room temperature (RT) crystal was formed on cooling via a rectangular columnar phase, which was absent during subsequent heating. [19] In the second case, the columnar monotropic phase was converted into another stable, columnar mesophase before reaching the RT crystalline phase. [20] Another interesting type of monotropic phase formed by HOBT-C8 molecules was studied by Cheng and co-workers, [21,22] who found an intermediate monotropic crystalline phase between a mesophase and a stable crystal. Some other examples of columnar monotropic phases were reported for non-conventional star-...