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由锰(II)产生的顺磁核磁共振弛豫机制:正交和四阶零场分裂项的作用。

The mechanism of paramagnetic NMR relaxation produced by Mn(II): role of orthorhombic and fourth-order zero field splitting terms.

作者信息

Sharp Robert

机构信息

Department of Chemistry, The University of Michigan, Ann Arbor, Michigan 48109-1055, USA.

出版信息

J Chem Phys. 2008 Oct 14;129(14):144307. doi: 10.1063/1.2981565.

Abstract

Mn(II) is a spin-5/2 paramagnetic ion that mediates a characteristically large NMR paramagnetic relaxation enhancement (NMR-PRE) of nuclear spins in solution. In the range of high magnetic field strengths (above about 0.3 T), where the electronic Zeeman interaction provides the largest term of the electron spin Hamiltonian, NMR relaxation mechanism is well understood. In the lower field range, the physical picture is more complex because of the presence in the spin Hamiltonian of zero field splitting (ZFS) terms that are comparable to or greater than the Zeeman term. This work describes a systematic study of the relaxation mechanism in the low field range, particularly aspects involving the dependence of NMR-PRE on the orthorhombic (E) and fourth-order (a(q)(4), q=0,2,4) ZFS tensor components. It is shown that the fourfold (a(4)(4)) and twofold (a(2)(4)) fourth-order components exert large orientation-dependent influences on the NMR-PRE. Thus, fourth-order terms with magnitudes equal to only a few percent of the quadratic ZFS terms (D,E) produce large changes in the shape of the magnetic field profile of the PRE. Effects arising from the orthorhombic quadratic ZFS term (E) are much smaller than those of the fourth-order terms and can in most cases be neglected. However, effects due to a(4)(4) and a(2)(4) need to be included in simulations of low field data.

摘要

锰(II)是一种自旋为5/2的顺磁性离子,它能介导溶液中核自旋的特征性大的核磁共振顺磁弛豫增强(NMR-PRE)。在高磁场强度范围(高于约0.3 T)内,电子塞曼相互作用提供了电子自旋哈密顿量的最大项,此时核磁共振弛豫机制已得到很好的理解。在低场范围内,物理图像更为复杂,因为自旋哈密顿量中存在与塞曼项相当或大于塞曼项的零场分裂(ZFS)项。这项工作描述了对低场范围内弛豫机制的系统研究,特别是涉及NMR-PRE对正交(E)和四阶(a(q)(4),q = 0,2,4)ZFS张量分量依赖性的方面。结果表明,四重(a(4)(4))和二重(a(2)(4))四阶分量对NMR-PRE产生很大的取向依赖性影响。因此,大小仅为二次ZFS项(D,E)百分之几的四阶项会使PRE的磁场分布形状产生很大变化。正交二次ZFS项(E)产生的影响远小于四阶项,在大多数情况下可以忽略。然而,在低场数据模拟中需要考虑a(4)(4)和a(2)(4)产生的影响。

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