Dedicated to Professor Gottfried Huttner on the occasion of his 68th birthdayMaterials that exhibit hysteretic bistability at temperatures not too far from ambient conditions are expected to have great potential for future memory or sensing applications. [1] The two relatively stable states should be clearly distinguished by their physical properties, such as their magnetic or optical characteristics. Thermal magnetic hysteresis with an abrupt and rapid property change around room temperature is particularly rare for molecule-based materials, [2] with spincrossover compounds providing the most prominent examples.[3] More recently, magnetic hysteresis has also been observed for some molecular organic radicals [4] or transition metal coordination compounds, [5,6] where switching between two states occurs through a thermal phase transition with orientational changes in the 3D crystal lattice. Herein, we report thermal hysteresis of the magnetic susceptibility for single crystals of the molecular dinickel(ii) complex [LNi 2 (N 3 ) 3 ] (1), in which a m 1,3 -azido ligand functions as an on/off switch for the intramolecular antiferromagnetic coupling between the two metal ions.Pyrazolate-based compartmental ligands such as L À , which bears thioether side-arms, have previously proven suitable as dinucleating scaffolds for the synthesis of preorganized azidonickel(ii) complexes that can serve as modules for the assembly of oligonuclear species or 1D extended chain compounds; [7] the bimetallic complex 1 was prepared as a potential building block in this context. Single crystals of 1 were grown from acetone/hexane, and an initial X-ray crystallographic analysis was carried out at 133 K (Figure 1).[8] As anticipated, both nickel ions in the C 2 -symmetric array are nested within their respective ligand compartment (with two sulfur and one nitrogen donors from the ligand side-arm) and are spanned by the bridging pyrazolate. A m 1,3 -azido bridge is found within the bimetallic pocket, and an additional terminal azide fills the remaining site at each of the six-coordinate metal ions.Since 1 did not exhibit any unusual structural features at this stage, the temperature dependence of its magnetic susceptibility was highly unexpected. The product c m T for a polycrystalline sample of 1 is depicted in Figure 2 for both decreasing and increasing temperature. The value of 1.82 cm 3 K mol À1 at 300 K is somewhat lower then the spinonly value expected for two uncoupled high-spin nickel(ii) ions (2.14 cm 3 K mol À1 for g = 2.07), and decreases only slightly upon lowering the temperature to 220 K. At 215 K, however, an abrupt drop of c m T occurs (centered at T fl = 212 K), followed by a much more rapid decline at lower temperatures; below 50 K c m T tends towards zero. The lowtemperature data are indicative of strong antiferromagnetic coupling and an S = 0 ground state, while coupling is apparently only weak above 220 K. c m T shows an analogous behavior when measured as a function of increasing temperature, but exhibits therma...