Isotropic Non-Heisenberg Behavior in M3(dpa)4Cl2 Extended Metal Atom Chains

被引:15
|
作者
Tabookht, Zahra [1 ]
Lopez, Xavier [1 ]
Benard, Marc [2 ]
de Graaf, Coen [1 ,3 ]
机构
[1] Univ Rovira & Virgili, Dept Quim Fis & Inorgan, Tarragona 43007, Spain
[2] CNRS ULP, UMR 7177 LC3, Lab Chim Quant, Inst Chim, Strasbourg, France
[3] Passeig Lluis Co, ICREA, Barcelona 08010, Spain
来源
JOURNAL OF PHYSICAL CHEMISTRY A | 2010年 / 114卷 / 46期
关键词
DENSITY-FUNCTIONAL THEORY; AB-INITIO; CONFIGURATION-INTERACTION; ELECTRON DELOCALIZATION; EXCHANGE INTERACTIONS; BONDING INTERACTION; ENERGY DIFFERENCES; CRYSTAL-STRUCTURES; STRING COMPLEXES; MOLECULAR WIRES;
D O I
10.1021/jp106038w
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Isotropic deviations to the standard Heisenberg Hamiltonian have been extracted for a series of trinuclear extended metal atom chain complexes, namely, [Ni-3(dpa)(4)Cl-2], and the hypothetical [NiPdNi(dpa)(4)Cl-2] and [Pd-3(dpa)(4)Cl-2], following a scheme recently proposed by Labeguerie and co-workers (J. Chem. Phys 2008, 129, 154110) within the density functional theory framework. Energy calculations of broken symmetry monodeterminantal solutions of intermediate M-s,M-tot values can provide an estimate of the magnitude of the biquadratic exchange interaction (lambda) that accounts for these deviations in systems with S = 1 magnetic sites. With the B3LYP functional, we obtain lambda = 1.37, 13.8, and 498 cm(-1) for the three molecules, respectively, meaning that a simple Heisenberg Hamiltonian is enough for describing the magnetic behavior of the Ni3 complex but definitely not for Pd-3. In the latter case, the origin of such extreme deviation arises from (i) an energetically affordable local non-Hund state (small intrasite exchange integral, K similar to 1960 cm(-1)) and (ii) a very effective overlap between Pd-4d orbitals and a large J. Furthermore, this procedure enables us to determine the relative weights of the two types of magnetic interactions, sigma- and delta-like, that contribute to the total magnetic exchange (J = J(sigma) + J(delta)). In all of the systems, J is governed by the a interaction by 95-98%.
引用
收藏
页码:12291 / 12298
页数:8
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