Manson J L, Lancaster T, Schlueter J A, Blundell S J, Brooks M L, Pratt F L, Nygren C L, Koo H-J, Dai D, Whangbo M-H
Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA. jmanson@ ewu.edu
Inorg Chem. 2007 Jan 8;46(1):213-20. doi: 10.1021/ic061590q.
The mixed-anion coordination polymer Cu(HCO2)(NO3)(pyz) was synthesized, its crystal structure was determined by X-ray diffraction, and its magnetic structure was characterized by ac susceptibility, dc magnetization, muon-spin relaxation, and spin dimer analysis. The crystal structure consists of five-coordinate Cu2+ ions that are connected through syn-anti bridging mu-HCO2- and mu-pyz ligands to form a highly corrugated two-dimensional layered network. Bulk magnetic measurements show a broad maximum in chi(T) at 6.6 K. The HCO2- and pyz ligands mediate ferromagnetic and antiferromagnetic spin exchange interactions between adjacent Cu2+ ions with the spin exchange parameters J/kB = 8.17 and -5.4 K, respectively (H = -JSigmaSi x Sj). The muon-spin relaxation data show a transition to a long-range magnetic ordering below TN = 3.66(3) K. For T < TN, the M(H) and chi'ac measurements provide evidence for a field-induced spin-flop transition at 15.2 kOe. That Cu(HCO2)(NO3)(pyz) undergoes a long-range magnetic ordering is an unexpected result because the one-dimensional Cu(NO3)2(pyz) and three-dimensional Cu(HCO2)2(pyz) compounds display linear chain antiferromagnetism with no long-range magnetic ordering down to 2 K.
合成了混合阴离子配位聚合物Cu(HCO2)(NO3)(pyz),通过X射线衍射确定了其晶体结构,并通过交流磁化率、直流磁化强度、μ子自旋弛豫和自旋二聚体分析对其磁结构进行了表征。晶体结构由五配位的Cu2+离子组成,这些离子通过顺-反桥连的μ-HCO2-和μ-pyz配体连接,形成高度起伏的二维层状网络。体磁测量表明,在6.6 K时χ(T)出现一个宽泛的最大值。HCO2-和pyz配体分别以自旋交换参数J/kB = 8.17和 -5.4 K介导相邻Cu2+离子之间的铁磁和反铁磁自旋交换相互作用(H = -JSigmaSi x Sj)。μ子自旋弛豫数据表明,在TN = 3.66(3) K以下转变为长程磁有序。对于T < TN,M(H)和χ'ac测量提供了在15.2 kOe处发生场诱导自旋翻转转变的证据。Cu(HCO2)(NO3)(pyz)发生长程磁有序是一个意外结果,因为一维的Cu(NO3)2(pyz)和三维的Cu(HCO2)2(pyz)化合物显示出线性链反铁磁性,在低至2 K时没有长程磁有序。