“…A single-molecule magnet (SMM) is broadly referred to the paramagnetic metal complex exhibiting magnetization blocking and slow relaxation of magnetization below a critical temperature, generally known as the blocking temperature, T B . , Due to the electronic spin-induced quantum magnetic states, SMMs inherit immense prospects in the high-impact modern technology such as high-density data storage, quantum computing, spintronics, bionics, multiferroics, and so forth. − However, the rational design and synthesis of potential SMMs are non-trivial. Since the discovery of the lanthanide (Ln) ion-based SMM behavior in phthalocyanine-sandwiched Ln(III) mononuclear complexes by Ishikawa et al, , there has been an insurgence of research interest in the arena of molecule-based magnetism associated with Ln ions. − Notably, large spin ground state and high magnetic anisotropy originating from strong spin–orbit coupling bequeath the Ln complexes, especially the Dy(III)-analogues, with fascinating slow magnetization dynamics when the Ln ions are complexed with appropriate crystal field (CF) environments. − Recent advances reveal that the Ln-based complexes with low coordination numbers and high CF symmetry are expected to exhibit a promising SMM behavior, especially for the lanthanide ions having oblate electrostatic potential surfaces corresponding to their ground magnetic microstates. ,− However, it is worth mentioning that the Ln ions prefer large coordination numbers, commonly 8–10, and variable coordination geometry because of their large ionic size and highly shielded valance (4 f ) orbitals. , At the same time, a subtle change in the coordination environment can influence the SMM behavior significantly. ,− ,− Therefore, having synthetic control over the inner coordination sphere with a desired CF topology is crucial in order for achieving potential SMMs rationally, especially for multinuclear SMMs.…”