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Giant Ising-Type Magnetic Anisotropy in Trigonal Bipyramidal Ni(Ⅱ) Complexes: Experiment and Theory

机译:三角双锥体Ni(Ⅱ)配合物中的巨伊辛型磁各向异性:实验和理论

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摘要

This paper reports the experimental and theoretical investigations of two trigonal bipyramidal Ni(Ⅱ) complexes, [Ni(Me_6tren)Cl]-(CIO_4) (1) and [Ni(Me_6tren)Br](Br) (2). High-field, high-frequency electron paramagnetic resonance spectroscopy performed on a single crystal of 1 shows a giant uniaxial magnetic anisotropy with an experimental D_(expt) value (energy difference between the M_s = ± 1 and M_s = 0 components of the ground spin state S = 1) estimated to be between -120 and -180 cm~(-1). The theoretical study shows that, for an ideally trigonal Ni(Ⅱ) complex, the orbital degeneracy leads to a first-order spin-orbit coupling that results in a splitting of the M_s = ± 1 and M_s = 0 components of approximately -600 cm~(-1). Despite the Jahn-Teller distortion that removes the ground term degeneracy and reduces the effects of the first-order spin-orbit interaction, the D value remains very large. A good agreement between theoretical and experimental results (theoretical D_(theor) between -100 and -200 cm~(-1)) is obtained.
机译:本文报道了两种三角双锥体Ni(Ⅱ)配合物[Ni(Me_6tren)Cl]-(CIO_4)(1)和[Ni(Me_6tren)Br](Br)(2)的实验和理论研究。对单晶1进行的高场,高频电子顺磁共振光谱显示了巨大的单轴磁各向异性,具有实验D_(expt)值(地旋转的M_s =±1和M_s = 0分量之间的能量差)状态S = 1)估计在-120至-180 cm〜(-1)之间。理论研究表明,对于理想的三角形Ni(Ⅱ)配合物,轨道的简并性会导致一阶自旋轨道耦合,从而导致M_s =±1和M_s = 0分量的分裂-600 cm 〜(-1)。尽管Jahn-Teller失真消除了地面项的简并性并减少了一阶自旋轨道相互作用的影响,但D值仍然很大。在理论和实验结果之间取得了很好的一致性(理论D_(理论)在-100和-200 cm〜(-1)之间)。

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  • 来源
    《Journal of the American Chemical Society》 |2013年第8期|3017-3026|共10页
  • 作者单位

    Laboratoire de Chimie et Physique Quantiques, Universite de Toulouse 3, 118 route de Narbonne, 31062 Toulouse cedex 06, France;

    Laboratoire de Chimie et Physique Quantiques, Universite de Toulouse 3, 118 route de Narbonne, 31062 Toulouse cedex 06, France,Department of Theoretical Chemistry, Zernike Institute for Advanced Materials, University of Groningen, The Netherlands,Departament de Quimica Fisica i Inorganica, Universitat Rovira i Virgili, Marcel.li Domingo s, 43007 Tarragona, Spain;

    Universite Paris Sud 11, CNRS, Institut de Chimie Moleculaire et des Materiaux d'Orsay, F-91405 Orsay, France;

    Laboratoire de Chimie et Physique Quantiques, Universite de Toulouse 3, 118 route de Narbonne, 31062 Toulouse cedex 06, France;

    Universite Paris Sud 11, CNRS, Institut de Chimie Moleculaire et des Materiaux d'Orsay, F-91405 Orsay, France;

    Laboratoire National des Champs Magnetiques Intenses, UPR CNRS 3228, Universite J. Fourier, 25, Avenue des Martyrs, B.P. 166, 38042 Grenoble Cedex 9, France;

    National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, United States;

    Universite de Lorraine, CRM2, UMR 7036, Boulevard des Aiguillettes, Vandoeuvre les Nancy, F-54506, France,CNRS, CRM2, UMR 7036, Boulevard des Aiguillettes, Vandoeuvre les Nancy, F-54506, France;

    Universite de Lorraine, CRM2, UMR 7036, Boulevard des Aiguillettes, Vandoeuvre les Nancy, F-54506, France,CNRS, CRM2, UMR 7036, Boulevard des Aiguillettes, Vandoeuvre les Nancy, F-54506, France;

    National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, United States,Department of Physics, Florida State University, Tallahassee, Florida 32306, United States;

    Universite Paris Sud 11, CNRS, Institut de Chimie Moleculaire et des Materiaux d'Orsay, F-91405 Orsay, France;

    Laboratoire de Chimie et Physique Quantiques, Universite de Toulouse 3, 118 route de Narbonne, 31062 Toulouse cedex 06, France;

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