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自由基配体场诱导的田边-菅野图的修正:Fe(II)-联氮自由基分子配合物的从头算研究

Modifications of Tanabe-Sugano Diagram Induced by Radical Ligand Field: Ab Initio Inspection of a Fe(II)-Verdazyl Molecular Complex.

作者信息

Roseiro Pablo, Yalouz Saad, Brook David J R, Ben Amor Nadia, Robert Vincent

机构信息

Laboratoire de Chimie Quantique, Institut de Chimie, CNRS/Université de Strasbourg, 4 rue Blaise Pascal, 67000 Strasbourg, France.

Department of Chemistry, San José State University, One Washington Square, San José, California 95192, United States.

出版信息

Inorg Chem. 2023 Apr 10;62(14):5737-5743. doi: 10.1021/acs.inorgchem.3c00275. Epub 2023 Mar 27.

Abstract

Quantum entanglement between the spin states of a metal center and radical ligands is suggested in an iron(II) [Fe(dipyvd)] compound (dipyvd = 1-isopropyl-3,5-dipyridil-6-oxoverdazyl). Wave function (Difference Dedicated Configuration Interaction, DDCI) inspections were carried out to stress the versatility of local spin states. We named this phenomenon , in reference to our previous work (see Roseiro et al., , e202200478) where we introduced the concept of as an extension of mesomerism to spin degrees of freedom. The construction of localized molecular orbitals allows for a reading of the wave functions and projections onto the local spin states. The low-energy spectrum is well-depicted by a Heisenberg picture. A 60 cm ferromagnetic interaction is calculated between the radical ligands with the = 0 and 1 states largely dominated by a local low-spin = 0. In contrast, the higher-lying = 2 states are superpositions of the local = 1 (17%, 62%) and = 2 (72%, 21%) spin states. Such mixing extends the traditional picture of a high-field Tanabe-Sugano diagram. Even in the absence of spin-orbit coupling, the avoided crossing between different local spin states is triggered by the field generated by radical ligands. This puzzling scenario emerges from versatile local spin states in compounds which extend the traditional views in molecular magnetism.

摘要

在一种铁(II)[Fe(dipyvd)]化合物(dipyvd = 1-异丙基-3,5-二吡啶基-6-氧代过氮自由基)中,金属中心的自旋态与自由基配体之间存在量子纠缠。进行了波函数(差分专用组态相互作用,DDCI)检查,以强调局部自旋态的多样性。参照我们之前的工作(见Roseiro等人, ,e202200478),我们将这种现象命名为 ,在之前的工作中我们引入了 概念,将其作为中介异构向自旋自由度的扩展。局域分子轨道的构建允许读取波函数并投影到局部自旋态上。低能谱由海森堡图像很好地描述。计算出在 = 0和1态的自由基配体之间存在60 cm的铁磁相互作用,主要由局部低自旋 = 0主导。相比之下,较高能级的 = 2态是局部 = 1(17%,62%)和 = 2(72%,21%)自旋态的叠加。这种混合扩展了高场田部-菅野图的传统图像。即使在没有自旋轨道耦合的情况下,不同局部自旋态之间的避免交叉也由自由基配体产生的场触发。这种令人困惑的情况源于化合物中多样的局部自旋态,它扩展了分子磁学的传统观点。

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