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Insertion of a single-molecule magnet inside a ferromagnetic lattice based on a 3D bimetallic oxalate network: Towards molecular analogues of permanent magnets

机译:在基于3D双金属草酸盐网络的铁磁晶格中插入单分子磁体:走向永磁体的分子类似物

摘要

The insertion of the single-molecule magnet (SMM) [MnIII(salen) (H2O)]2 2+ (salen2-=N,N-ethylenebis- (salicylideneiminate)) into a ferromagnetic bimetallic oxalate network affords the hybrid compound [MnIII(salen)(H2O)] 2[MnIICrIII(ox)3] 2×(CH3OH)×(CH3CN)2 (1). This cationic Mn2 cluster templates the growth of crystals formed by an unusual achiral 3D oxalate network. The magnetic properties of this hybrid magnet are compared with those of the analogous compounds [Mn III(salen)(H2O)]2[ZnIICr III(ox)3]2×(CH3OH) ×(CH3CN)2 (2) and [InIII(sal 2-trien)][MnIICrIII(ox)3] ×(H2O)0.25×(CH3OH) 0.25×(CH3CN)0.25 (3), which are used as reference compounds. In 2 it has been shown that the magnetic isolation of the Mn2 clusters provided by their insertion into a paramagnetic oxalate network of CrIII affords a SMM behavior, albeit with blocking temperatures well below 500 mK even for frequencies as high as 160 kHz. In 3 the onset of ferromagnetism in the bimetallic MnIICrIII network is observed at Tc=5 K. Finally, in the hybrid compound 1 the interaction between the two magnetic networks leads to the antiparallel arrangement of their respective magnetizations, that is, to a ferrimagnetic phase. This coupling induces also important changes on the magnetic properties of 1 with respect to those of the reference compounds 2 and 3. In particular, compound 1 shows a large magnetization hysteresis below 1 K, which is in sharp contrast with the near-reversible magnetizations that the SMMs and the oxalate ferromagnetic lattice show under the same conditions. Magnetic couple: The insertion of a single-molecule magnet (SMM) into a ferromagnetic bimetallic oxalate network affords the hybrid compound [MnIII(salen)(H 2O)]2[MnIICrIII(ox) 3]2×(MeOH)3×(H2O). The interaction between the two magnetic networks leads to the antiparallel arrangement of their respective magnetizations (see figure). This coupling induces a large magnetization hysteresis below 1 K, in sharp contrast with the near-reversible magnetizations that the SMMs and the oxalate ferromagnetic lattice show under the same conditions. Copyright © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.
机译:将单分子磁体(SMM)[MnIII(salen)(H2O)] 2 2+(salen2- = N,N-亚乙基双-(水杨亚胺))插入铁磁双金属草酸盐网络中可得到杂化化合物[MnIII( Salen)(H 2 O)] 2 [MnIICrIII(ox)3] 2×(CH 3 OH)×(CH 3 CN)2(1)。这种阳离子Mn2簇可模板化由不寻常的非手性3D草酸酯网络形成的晶体的生长。将此杂化磁体的磁性与类似化合物[Mn III(salen)(H2O)] 2 [ZnIICr III(ox)3] 2×(CH3OH)×(CH3CN)2(2)和[InIII (盐2-三烯)] [MnIICrIII(ox)3]×(H2O)0.25×(CH3OH)0.25×(CH3CN)0.25(3),用作参考化合物。在图2中,已经表明,通过将Mn2团簇插入CrIII的顺磁性草酸盐网络中而提供的磁隔离提供了SMM行为,尽管即使对于高达160 kHz的频率,阻断温度也远低于500 mK。在图3中,在Tc = 5 K处观察到双金属MnIICrIII网络中铁磁性的开始。最后,在混合化合物1中,两个磁网络之间的相互作用导致各自磁化强度的反平行排列,即形成亚铁磁相。相对于参考化合物2和3的这种耦合,还引起了1的磁性的重要变化。特别是化合物1在1 K以下显示出较大的磁滞,这与几乎可逆的磁化形成鲜明对比。 SMM和草酸盐铁磁晶格在相同条件下显示。磁偶:将单分子磁体(SMM)插入铁磁性双金属草酸盐网络中可得到杂化化合物[MnIII(salen)(H 2O)] 2 [MnIICrIII(ox)3] 2×(MeOH)3×( H2O)。两个磁网络之间的相互作用导致它们各自磁化强度的反平行排列(见图)。这种耦合在1 K以下引起较大的磁化磁滞,这与SMM和草酸盐铁磁晶格在相同条件下表现出的近可逆磁化形成鲜明对比。版权所有©2014 WILEY-VCH Verlag GmbH&Co.KGaA,Weinheim。

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