Herein we report the synthesis and structures of [(CH3)2NH2]Er(HCO2)2(C2O4) and [(NH2)3C]Er(HCO2)2(C2O4), in which the inclusion of divalent oxalate ligands allows for the exclusive incorporation of A+ and B3+ cations in...

This work reports a new series of ALn(HCO2)(C2O4)1.5 (A=[(CH3)2NH2]+ and Ln3+=Tb3+‐Er3+) compounds made solvothermally. These Cmce phases combine monovalent and divalent ligands, which enables a scarce combination of A+ and B3+ cations in a hybrid perovskite‐like compound. The ratio of ligands leads to ordered anion vacancies, which alternate with oxalate linkers along the c‐axis. The A‐site cations are disordered and cannot be identified crystallographically, likely a result of the larger pores of these frameworks compared to the recently reported AEr(HCO2)2(C2O4) phases. Neutron and infrared spectroscopy, supported by elemental composition, enables these cations to be identified as [(CH3)2NH2]+ molecules. Magnetic property measurements suggest these materials have weak antiferromagnetic interactions but remain paramagnetic to 1.8 K.

In recent years there has been tremendous interest in perovskite-like ABX3 hybrid frameworks, built from inorganic and organic building blocks, for their semiconducting, ferroelectric and magnetic properties. Much of the attraction in these materials lies in the well-known chemical flexibility of perovskite structures, which allows them to accommodate a wide range of cations and anions, as is well known perovskite oxides. Much of this flexibility is enhanced in inorganic-organic perovskites both with respect to their chemistry e.g. their ability to incorporate a wide range of molecular A-site cations and ligands, distortion modes and mechanical flexibility. In one key aspect, however, hybrid perovskites currently have less flexibility compared to conventional perovskites, namely the range of formal charges of cations they can incorporate. This results from the ligands in these hybrid material almost always being monovalent, which essentially restricts the A and B sites to monovalent and divalent cations, respectively.Recent work in our group has realised a combination of monovalent and divalent ligands in perovskite-like materials via replacing HCO2linker with C2O4 2ligands. Most interestingly this has yielded [(CH2)3N]Er(HCO2)2(C2O4) and [(CH3)2NH2]Er(HCO2)2(C2O4), allowing monovalent organic A-site and trivalent B-site cations to be combined for the first time in a stoichiometric ABX3 perovskite. Our presentation will discuss the synthesis, crystal structures and magnetic properties of these materials. These exhibit A-site cation ordering up to 500 K, which will likely make related phases of interest as ferroelectrics. The greater framework flexibility in [(CH2)3N]Er(HCO2)2(C2O4) leads to it exhibiting significant anisotropic negative thermal expansion while the more rigid [(CH 3 ) 2 NH 2 ]Er(HCO 2 ) 2 (C 2 O 4 ) phase does not.The second part of our presentation will focus on the related ALn(C2O4)1.5(HCO2) (Ln = Tb-Er) phases, where we find that replacing an additional formate ligand with oxalate leads to a structure with ordered ligand vacancies. This leads to larger channels in the materials, which is likely the cause of the disorded A-site cations in these materials; ultimately the presence and nature of these A-site cations, which could not be identified crystallographically, have been confirmed by neutron and infrared spectroscopy. These two new series of materials highlight the potential to expand the flexibility of hybrid perovskite and perovskite-like materials by incorporating divalent ligands, allowing their properties to be further tailored for applications.

The Cover Feature shows the analysis of a new series of ALn(HCO2)(C2O4)1.5 compounds, which are rare examples of hybrid perovskite‐like structures with ordered anion vacancies and trivalent lanthanide cations. The highly disordered A‐site contents were confirmed as [(CH3)2NH2]+ molecules, using a combination of neutron and IR spectroscopy. Image Credit: Thomas J. Hitchings (University of Kent). More information can be found in the Full Paper by P. J. Saines and co‐workers.