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高自旋四配位二酮亚胺铁(II)配合物的穆斯堡尔谱、电子顺磁共振及理论研究

Mössbauer, electron paramagnetic resonance, and theoretical study of a high-spin, four-coordinate Fe(II) diketiminate complex.

作者信息

Stoian Sebastian A, Smith Jeremy M, Holland Patrick L, Münck Eckard, Bominaar Emile L

机构信息

Department of Chemistry, Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA.

出版信息

Inorg Chem. 2008 Oct 6;47(19):8687-95. doi: 10.1021/ic8004568. Epub 2008 Sep 10.

Abstract

The iron(II) complex LFeCl 2Li(THF) 2 (L = beta-diketiminate), 1, has been studied with variable-temperature, variable-field Mossbauer spectroscopy and parallel mode electron paramagnetic resonance (EPR) spectroscopy in both solution and the solid state. In zero applied field the 4.2 K Mossbauer spectrum exhibits an isomer shift delta = 0.90 mm/s and quadrupole splitting Delta E Q = 2.4 mm/s, values that are typical for the high-spin ( S = 2) state anticipated for the iron in 1. Spectra recorded in applied magnetic fields yield an anisotropic magnetic hyperfine tensor with A x = +2.3 (+ 1.0) T, A y = A z = -21.5 T ( solution) and a nearly axial zero-field splitting of the spin quintet with D = D x approximately -14 cm (-1) and rhombicity E/ D approximately 0.1. The small, positive value for A x results from the presence of residual orbital angular momentum along x. The EPR analysis gives g x approximately 2.4 (and g y approximately g z approximately 2.0) and reveals a split " M S = +/- 2" ground doublet with a gap distributed around Delta = 0.42 cm (-1). The Mossbauer spectra of 1 show unusual features that arise from the presence of orientation-dependent relaxation and a distribution in the magnetic hyperfine field along x. The origin of the distribution has been analyzed using crystal field theory. The analysis indicates that the distribution in the magnetic hyperfine field originates from a narrow distribution, sigma phi approximately 0.5 degrees , in torsion angle phi between the FeN 2 and FeCl 2 planes, arising from minute inhomogeneities in the molecular environments.

摘要

已采用变温、变场穆斯堡尔光谱以及溶液和固态下的平行模式电子顺磁共振(EPR)光谱对铁(II)配合物LFeCl₂Li(THF)₂(L = β - 二酮亚胺),即1进行了研究。在零外场下,4.2 K时的穆斯堡尔光谱显示出同质异能位移δ = 0.90 mm/s和四极分裂ΔEQ = 2.4 mm/s,这些值对于1中铁预期的高自旋(S = 2)态来说是典型的。在施加磁场下记录的光谱产生了一个各向异性的磁超精细张量,其中Ax = +2.3(±1.0)T,Ay = Az = -21.5 T(溶液),以及自旋五重态的近轴向零场分裂,D = Dx ≈ -14 cm⁻¹且菱形度E/D ≈ 0.1。Ax的小正值是由于沿x方向存在残余轨道角动量。EPR分析得出gx ≈ 2.4(且gy ≈ gz ≈ 2.0),并揭示了一个分裂的“MS = ±2”基态二重态,其能隙分布在Δ = 0.42 cm⁻¹左右。1的穆斯堡尔光谱显示出由取向依赖弛豫以及沿x方向磁超精细场的分布所产生的异常特征。已使用晶体场理论分析了该分布的起源。分析表明,磁超精细场的分布源于FeN₂和FeCl₂平面之间扭转角φ的窄分布,σφ ≈ 0.5°,这是由分子环境中的微小不均匀性引起的。

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