Bastardis Roland, Guihéry Nathalie, de Graaf Coen
Laboratoire de Chimie et de Physique Quantiques, IRSAMC/UMR5626, Universite Paul Sabatier, 118 Route de Narbonne, F-31062 Toulouse Cedex 4, France.
J Chem Phys. 2008 Sep 14;129(10):104102. doi: 10.1063/1.2975336.
This paper analyzes the different contributions to the magnetic coupling in systems with more than one unpaired electron per center. While in S=12 spin systems the Heisenberg Hamiltonian involving only bilinear exchange interactions is reliable for the description of the magnetic states, biquadratic exchange interactions must be sometimes introduced for S=1 (or higher) spin systems to account for isotropic deviations to Heisenberg behavior. The analysis establishes that the excited atomic states, the so-called non-Hund states, are responsible for the main contribution to the deviations. The kinetic exchange contribution and the spin, hole, and particle polarizations increase the magnetic coupling but essentially maintain the Heisenberg pattern. The importance of the different contributions has been studied for a series of Ni(2) compounds with a polarizable double azido bridge. The coupling between two Fe(3+) ions in the molecular crystal Na(3)FeS(3), which is known experimentally to present large deviations to Heisenberg behavior, has also been investigated.
本文分析了每个中心有多个未成对电子的系统中对磁耦合的不同贡献。对于(S = \frac{1}{2})自旋系统,仅涉及双线性交换相互作用的海森堡哈密顿量对于描述磁态是可靠的,而对于(S = 1)(或更高)自旋系统,有时必须引入双二次交换相互作用以解释对海森堡行为的各向同性偏差。分析表明,激发的原子态,即所谓的非洪德态,是偏差的主要贡献来源。动力学交换贡献以及自旋、空穴和粒子极化增加了磁耦合,但基本上保持了海森堡模式。对于一系列具有可极化双叠氮桥的镍(II)化合物,研究了不同贡献的重要性。还研究了分子晶体(Na_3FeS_3)中两个(Fe^{3 +})离子之间的耦合,实验已知该耦合对海森堡行为有很大偏差。