Triki Smaïl, Gómez-García Carlos J, Ruiz Eliseo, Sala-Pala Jean
UMR CNRS 6521, University of Bretagne Occidentale, 6 avenue V. Le Gorgeu, BP 809, 29285 Brest Cedex, France.
Inorg Chem. 2005 Jul 25;44(15):5501-8. doi: 10.1021/ic0504543.
Reaction of NaN(3) with the Cu(II)(tn) ion (tn = 1,3-diaminopropane) in basic aqueous solution yields the azido-bridged complex of formula [Cu(2)(tn)(2)(N(3))(4)] (1), which is characterized by X-ray crystallography. The structure of 1 is made up of dinuclear neutral complexes, of formula [Cu(2)(tn)(2)(N(3))(4)], resulting from the assembling of two mononuclear units through two equivalent end-on azide bridges connecting asymmetrically two Cu(tn)(N(3))(2) entities. These dinuclear units are connected through two asymmetric end-to-end N(3) bridges to form a chain of dimers. Magnetic measurements for compound 1 show weak antiferromagnetic exchange interactions between the Cu(II) ions. The magnetic data were modeled using the susceptibility expression derived for an alternating AF S = 1/2 chain. A very satisfactory fit over the whole temperature range was obtained with g = 2.1438(4), J(1) = -3.71(2) cm(-1), and J(2) = -3.10(2) cm(-1) (J(1) and J(2) are the singlet-triplet separations). This magnetic behavior differs from those observed for similar examples which were reported as having alternating ferro- and antiferromagnetic exchange interactions; thus, DFT calculations were done to understand the nature of the magnetic coupling in such asymmetric end-on and end-to-end N(3) bridges. Theoretical results show that the double asymmetric end-on bridges produce antiferromagnetic coupling while the end-to-end ones can present ferro- or antiferromagnetic coupling depending on the copper coordination sphere.
叠氮化钠(NaN₃)与[Cu(II)(tn)]²⁺离子(tn = 1,3 - 二氨基丙烷)在碱性水溶液中反应生成化学式为[Cu₂(tn)₂(N₃)₄]的叠氮桥联配合物(1),该配合物通过X射线晶体学进行表征。1的结构由化学式为[Cu₂(tn)₂(N₃)₄]的双核中性配合物组成,它是由两个单核单元通过两个等效的端连叠氮桥不对称地连接两个Cu(tn)(N₃)₂实体组装而成。这些双核单元通过两个不对称的端对端N₃桥相连形成二聚体链。化合物1的磁性测量表明Cu(II)离子之间存在弱反铁磁交换相互作用。利用为交替AF S = 1/2链推导的磁化率表达式对磁性数据进行建模。在整个温度范围内获得了非常令人满意的拟合结果,g = 2.1438(4),J₁ = -3.71(2) cm⁻¹,J₂ = -3.10(2) cm⁻¹(J₁和J₂是单重态 - 三重态分离)。这种磁性行为与报道的具有交替铁磁和反铁磁交换相互作用的类似例子所观察到的不同;因此,进行了DFT计算以了解这种不对称端连和端对端N₃桥中磁耦合的性质。理论结果表明,双不对称端连桥产生反铁磁耦合,而端对端桥根据铜的配位球情况可呈现铁磁或反铁磁耦合。