Calix[4]arene Based Single-Molecule Magnets** Georgios Karotsis, Simon J. Teat, Wolfgang Wernsdorfer, Stergios Piligkos, Scott J. Dalgarno* and Euan K. Brechin* Mr. G. Karotsis, Dr. E. K. Brechin, School of Chemistry, The University of Edinburgh, West Mains Road, Edinburgh, EH9 3JJ, UK. Fax: (+44)-131-650-6453 E-mail: ebrechin@staffmail.ed.ac.uk Dr. S. J. Dalgarno, School of Engineering and Physical Sciences, Heriot-Watt University, Riccarton, Edinburgh, EH14 4AS. Fax: (+44)-131-451-3180 E-mail: S.J.Dalgarno@hw.ac.uk Prof. Dr. W. Wernsdorfer, Institut Neel, CNRS, Grenoble Cedex 9, France. Dr. S. Piligkos, Department of Chemistry, University of Copenhagen, Universitetsparken 5, DK-2100, Denmark. Dr. S. J. Teat, Advanced Light Source, Berkeley Laboratory, 1 Cyclotron Road, MS6R2100, Berkeley, CA 94720, USA. The Advanced Light Source is supported by the Director, Office of Science, Office of Basic Energy Sciences, of the US Department of Energy under contract no. DE-AC02-05CH11231. Single-molecule magnets (SMMs) [1] have been the subject of much interest in recent years because their molecular nature and inherent physical properties allow the crossover between classical and quantum physics to be observed. [2] The macroscopic observation of quantum phenomena - tunneling between different spin states, [3] quantum interference between tunnel paths [4] - not only allows scientists to study quantum mechanical laws in great detail, but also provides model systems with which to investigate the possible implementation of spin- based solid state qubits [5] and molecular spintronics. [6] The isolation of small, simple SMMs is therefore an exciting prospect. To date almost all SMMs have been made via the self-assembly of 3d metal ions in the presence of bridging/chelating organic ligands. [7] However, very recently an exciting new class of SMMs, based on 3d metal clusters (or single lanthanide ions) housed within polyoxometalates, [8] has appeared. These types of molecule, in which the SMM is completely encapsulated within (or shrouded by) a “protective” organic or inorganic sheath have much potential for design and manipulation: for example, for the removal of unwanted dipolar interactions, the introduction of redox activity, or to simply aid functionalisation for surface grafting. [9] Calix[4]arenes are cyclic (typically bowl-shaped) polyphenols that have been used extensively in the formation of versatile self-assembled supramolecular structures. [10] Although many have been reported, p- t But-calix[4]arene and calix[4]arene (TBC4 and C4 respectively, Figure 1A) are frequently encountered due to a) synthetic accessibility, and b) vast potential for alteration at either the upper or lower rim of the macrocyclic framework. [11] Within the field of supramolecular chemistry, TBC4 is well known for interesting polymorphic behavior and phase transformations within anti-parallel bi-layer arrays, while C4 often forms self-included trimers. [12] The polyphenolic nature of calix[n]arenes (where n = 4 – 8) also suggests they should be excellent candidates as ligands for the isolation of molecular magnets, but to date their use in the isolation of paramagnetic cluster compounds is rather limited. [13] Herein we present the first Mn cluster and the first SMM to be isolated using any methylene bridged calix[n]arene - a ferromagnetically coupled mixed-valence [Mn III2 Mn II2 ] complex housed between either two TBC4s or two C4s. Reaction of MnBr 2 with TBC4 and NEt 3 in a solvent mixture of MeOH/DMF results in the formation of the complex [Mn III2 Mn II2 (OH) 2 (TBC4) 2 (DMF) 6 ] (1) which crystallises as purple blocks that are in the monoclinic space group P2 1 /c. The cluster (Figure 1B) comprises a planar diamond or butterfly-like [Mn III2 Mn II2 (OH) 2 ] core in which the wing tip Mn ions (Mn1) are in the 3+ oxidation state and the body Mn ions (Mn2) in the 2+ oxidation state. This is a common structural type in Mn SMM chemistry, [14] but the oxidation state distribution here is highly unusual, being “reversed” from the norm in which the body Mn ions are almost always 3+. Indeed the “reversed” core has been seen only once before, in the cluster [Mn III2 Mn II2 (teaH) 2 (acac) 4 (MeOH) 2 ] 2+ (2) (teaH 3 = triethanolamine) and its analogues. [15] The Mn 3+ ions are in distorted octahedral geometries with the Jahn-Teller axes defined by O5(DMF)-Mn1-O6(OH). The four equatorial sites are occupied by the oxygen atoms (O1-O4) of the TBC4, two of which bridge in a µ 2 -fashion to the central Mn 2+ ions (Mn1-O4-Mn2, 103.5°; Mn1-O1-Mn2, 105.4°). These are connected to each other (Mn2-O6-Mn2’, 94.7°) and to the Mn 3+ ions (Mn1-O6-Mn2, 100.4°; Mn1- O6-Mn2’, 98.8°) via two µ 3 -bridging OH - ions, with the two remaining equatorial sites (completing the distorted octahedral geometry on Mn2) filled by terminal DMF molecules. There are no inter-molecular H-bonds between symmetry equivalents of 1, with the closest
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