Ren X M, Okudera H, Kremer R K, Song Y, He C, Meng Q J, Wu P H
Coordination Chemistry Institute & State Key Laboratory and Department of Electronic Science & Engineering, Nanjing University, Nanjing 210093, People's Republic of China.
Inorg Chem. 2004 Apr 19;43(8):2569-76. doi: 10.1021/ic035405+.
Three ion pair complexes, [4-R-benzylpyridinium][bis(maleodinitriledithiolato)platinum(III)] (abbreviated as [RBzPy][Pt(mnt)(2)]; R = Cl (1), Br (2), or NO(2) (3)), have been synthesized. The cations and anions stack into well-separated columns in the solid state, and the Pt(III) ions form a 1-D zigzag chain within a Pt(mnt)(2) column through Pt...S, S...S, and Pt...S...Pt interactions. The chain is uniform in 1 and 2, while it alternates in 3. Unusual magnetic phase transitions from paramagnetism to diamagnetism were observed in these three complexes at approximately 275 K for 1, approximately 269 K for 2, and approximately 184 K for 3. These phase transitions were also found in DSC measurements for 1 and 2. The overall magnetic behaviors for 1-3 indicate the presence of antiferromagnetic exchange interactions in the high-temperature phase and spin-gapped systems in the low-temperature phase. Below 50 K, 2 exhibits weak ferromagnetism. The spontaneous moments are nearly repressed by a field of 1.0 T. The crystal structure of 2 at 173 K reveals that there are two crystallographically independent Pt(mnt)(2) entries in an asymmetric unit. These two crystallographically independent Pt(mnt)(2) entries satisfy the spin-canting condition, and the EPR spectra measured at room temperature exhibit anisotropic character. Therefore, the weak ferromagnetic behavior in the low-temperature region for 2 can be attributed to the spin-canting phenomenon.
合成了三种离子对配合物,即[4-R-苄基吡啶鎓][双(马来二腈二硫醇根)铂(III)](简称为[RBzPy][Pt(mnt)₂];R = Cl (1)、Br (2) 或 NO₂ (3))。阳离子和阴离子在固态下堆积成间隔良好的柱状结构,并且Pt(III)离子通过Pt…S、S…S和Pt…S…Pt相互作用在[Pt(mnt)₂]⁻柱内形成一维锯齿链。该链在1和2中是均匀的,而在3中交替。在这三种配合物中观察到了不寻常的从顺磁性到抗磁性的磁相变,1大约在275 K,2大约在269 K,3大约在184 K。在1和2的差示扫描量热法测量中也发现了这些相变。1 - 3的整体磁行为表明在高温相中存在反铁磁交换相互作用,在低温相中存在自旋能隙系统。在50 K以下,2表现出弱铁磁性。自发磁矩几乎被1.0 T的磁场抑制。2在173 K时的晶体结构表明,在一个不对称单元中有两个晶体学独立的[Pt(mnt)₂]⁻项。这两个晶体学独立的[Pt(mnt)₂]⁻项满足自旋倾斜条件,并且在室温下测量的电子顺磁共振光谱表现出各向异性特征。因此,2在低温区域的弱铁磁行为可归因于自旋倾斜现象。