Studying the self-assembly of molecules at the solution/solid interface (SSI) provides unique insight into bottom-up molecular architectures, which have applications varying from solar conversion [1][2][3] and electronic devices [4][5][6][7] to providing insight into fundamental biological mechanisms. [8,9] The investigation of molecular organization at the SSI is largely conducted via scanning tunnelling microscopy (STM), which can be used to directly visualize molecular kinetics and geometries in situ. [10][11][12][13][14] The development of this technique has provided unprecedented access to the details of surface molecular self-assembly. [15,16] The Gibbs free energy for molecular systems at the SSI comprises an enthalpic contribution dominated by the interaction energies of the adsorbed species (intermolecular and molecule-substrate) and an entropic component primarily associated with the molecules in solution. The details of the energy balance are quite subtle, and the level of ab initio predictive power necessary for the ground-up design of molecular networks remains elusive. However, empirical heuristics describing the interplay of physisorption, molecule-molecule interaction, solvent and concentration effects are emerging from carefully-controlled experiments. [17][18][19][20] Until recently, temperature was the only variable in the Gibbs free energy expression that had not been systematically varied, even though it has implications for both thermodynamics and kinetics, as well as for critical parameters like solubility and viscosity. We highlight here the first few reports of temperature control in SSI-STM experiments.The infrastructure required to modify an existing STM for temperature control is modest, and designs can be easily adapted from add-on stages originally intended for commercial atomic force microscopy. [21][22][23] In general, temperatures above room temperature are achieved by inserting either a small heater [24,25] or a thermoelectric (Peltier) device [26] under the sample. The latter is the more versatile solution, since driving current in the opposite direction through the Peltier device results in cooling. In either case, the temperature at the sample must be monitored with a thermocouple or similar, and the heater should ideally be controlled via a proportional-integral-derivative (PID) algorithm.The first temperature-controlled SSI-STM study was reported by English and Hipps, who imaged coronene at the heptanoic acid/Au(111) interface at temperatures up to 558C. [24] This early work established a proof-of-principle, and has since been followed by examples of temperature control in SSI-STM designed to systematically elucidate the energetics of SSI self-assembly.In an elegant illustration of the principle of closest packing, [27,28] Marie et al. showed that in increasing from room temperature to 508C, hexakis(n-dodecyl)-perihexabenzocoronene (HBC-C 12 ) at the n-tetradecane/Au(111) interface undergoes successive, irreversible phase transitions that increase its density of packing (Fi...