Rams Michał, Tomkowicz Zbigniew, Böhme Michael, Plass Winfried, Suckert Stefan, Werner Julia, Jess Inke, Näther Christian
Institute of Physics, Jagiellonian University, Łojasiewicza 11, 30-348 Kraków, Poland.
Institut für Anorganische und Analytische Chemie, Universität Jena, Humboldtstr. 8, 07743 Jena, Germany.
Phys Chem Chem Phys. 2017 Jan 25;19(4):3232-3243. doi: 10.1039/c6cp08193b.
Two new transition metal thiocyanate coordination polymers with the composition [Co(NCS)(4-vinylpyridine)] (1) and [Co(NCS)(4-benzoylpyridine)] (2) were synthesized and their crystal structures were determined. In both compounds the Co cations are octahedrally coordinated by two trans-coordinating 4-vinyl- or 4-benzoylpyridine co-ligands and four μ-1,3-bridging thiocyanato anions and linked into chains by the anionic ligands. While in 1 the N and the S atoms of the thiocyanate anions are also in trans-configuration, in 2 they are in cis-configuration. A detailed magnetic study showed that the intra-chain ferromagnetic coupling is slightly stronger for 2 than for 1, and that the chains in both compounds are weekly antiferromagnetically coupled. Both compounds show a long range magnetic ordering transition at T = 3.9 K for 1 and T = 3.7 K for 2, which is confirmed by specific heat measurements. They also show a metamagnetic transition at a critical field of 450 Oe (1) and 350 Oe (2), respectively. Below T1 and 2 exhibit magnetic relaxations resembling relaxations of single chains. The exchange constants obtained from magnetic and specific heat data are in good accordance with those obtained from constrained DFT calculations carried out on isolated model systems. The ab initio calculations allowed us to find the principal directions of anisotropy.
合成了两种新的硫氰酸过渡金属配位聚合物,其组成为[Co(NCS)(4-乙烯基吡啶)](1)和[Co(NCS)(4-苯甲酰基吡啶)](2),并测定了它们的晶体结构。在这两种化合物中,Co阳离子由两个反式配位的4-乙烯基或4-苯甲酰基吡啶共配体和四个μ-1,3-桥连硫氰酸根阴离子八面体配位,并通过阴离子配体连接成链。在1中硫氰酸根阴离子的N和S原子也处于反式构型,而在2中它们处于顺式构型。详细的磁性研究表明,2中链内铁磁耦合比1略强,且两种化合物中的链均为弱反铁磁耦合。两种化合物在T = 3.9 K(1)和T = 3.7 K(2)时均显示出长程磁有序转变,这通过比热测量得到证实。它们还分别在450 Oe(1)和350 Oe(2)的临界场处显示出变磁转变。在T1以下,1和2表现出类似于单链弛豫的磁弛豫。从磁性和比热数据获得的交换常数与在孤立模型系统上进行的受限密度泛函理论计算得到的结果非常吻合。从头算计算使我们能够找到各向异性的主方向。