Wöhlert Susanne, Tomkowicz Zbigniew, Rams Michał, Ebbinghaus Stefan G, Fink Lothar, Schmidt Martin U, Näther Christian
Institut für Anorganische Chemie, Christian-Albrechts-Universität zu Kiel , Max-Eyth-Straße 2, 24118 Kiel, Germany.
Inorg Chem. 2014 Aug 18;53(16):8298-310. doi: 10.1021/ic500572p. Epub 2014 Jul 31.
Reaction of Co(NCS)2 with 1,2-bis(4-pyridyl)-ethane (bpa) leads to the formation of [Co(NCS)2(bpa)2]n, which, on heating, transforms into the new layered coordination polymer [Co(NCS)2(bpa)]n. This compound can also be prepared in solution, but because no reasonable single crystals are available, its crystal structure was determined from X-ray powder data from scratch. In the crystal structure of [Co(NCS)2(bpa)]n, the cobalt(II) cations are coordinated by two S-bonded and two N-bonded thiocyanato anions and two N atoms of the bpa co-ligands in a distorted octahedral geometry. The cobalt(II) cations are linked into chains by pairs of μ-1,3 bridging thiocyanato anions. These chains are further connected into layers by the 1,2-bis(4-pyridyl)-ethane ligand. The compound was magnetically characterized, and, for comparative purposes, the complementary magnetic study of a known and very similar compound, [Co(NCS)2(bpe)]n (bpe = 1,2-bis(4-pyridyl)-ethylene), was also undertaken. The compounds differ in their interchain interactions, which are antiferromagnetic but significantly greater for [Co(NCS)2(bpe)]n. Magnetic measurements indicate that [Co(NCS)2(bpa)]n is a canted antiferromagnet with Néel temperature TN = 3.1 K and that Co(NCS)2(bpe) is an antiferromagnet with TN = 4.0 K. Both compounds show a metamagnetic transition with a critical field HC ∼ 40 Oe and ∼ 400 Oe, respectively. Magnetic relaxations were studied by means of dc and ac methods and analyzed using the Argand diagrams. Except for the thermally activated single chain and domain wall relaxations observed for both compounds, temperature-independent slow relaxations were observed for [Co(NCS)2(bpa)]n.
二硫氰酸钴(II)与1,2 - 双(4 - 吡啶基)乙烷(bpa)反应生成[Co(NCS)₂(bpa)₂]ₙ,加热时,其转变为新的层状配位聚合物[Co(NCS)₂(bpa)]ₙ。该化合物也可在溶液中制备,但由于没有合适的单晶,其晶体结构从头开始由X射线粉末数据确定。在[Co(NCS)₂(bpa)]ₙ的晶体结构中,钴(II)阳离子由两个硫键合和两个氮键合的硫氰酸根阴离子以及双齿配体bpa的两个氮原子以扭曲的八面体几何构型配位。钴(II)阳离子通过μ - 1,3桥连硫氰酸根阴离子对连接成链。这些链通过1,2 - 双(4 - 吡啶基)乙烷配体进一步连接成层。对该化合物进行了磁性表征,为作比较,还对一种已知且非常相似的化合物[Co(NCS)₂(bpe)]ₙ(bpe = 1,2 - 双(4 - 吡啶基)乙烯)进行了补充磁性研究。这两种化合物的链间相互作用不同,均为反铁磁性,但[Co(NCS)₂(bpe)]ₙ的链间相互作用明显更强。磁性测量表明,[Co(NCS)₂(bpa)]ₙ是一种倾斜反铁磁体,奈尔温度TN = 3.1 K,而Co(NCS)₂(bpe)是一种奈尔温度TN = 4.0 K的反铁磁体。两种化合物均表现出变磁转变,临界场HC分别约为40 Oe和约400 Oe。通过直流和交流方法研究了磁弛豫,并使用阿尔冈图进行分析。除了两种化合物均观察到的热激活单链和畴壁弛豫外,[Co(NCS)₂(bpa)]ₙ还观察到与温度无关的缓慢弛豫。