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Tuning Anisotropy Barriers in a Family of Tetrairon(III) Single-Molecule Magnets with an S = 5 Ground State

机译:调谐具有S = 5基态的四铁(III)单分子磁体族的各向异性势垒

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摘要

Tetrairon(III) Single-Molecule Magnets (SMMs) with a propeller-like structure exhibit tuneable magnetic anisotropy barriers in both height and shape.The clusters [Fe_4(L~1)_2(dpm)_6] (1),[Fe_4(L~2)_2(dpm)_6] (2),[Fe4(L~3)_2(dpm)6] centre dot Et_2O (3 centre dot Et_2O),and [Fe_4(OEt)_3(L~4)(dpm)_6] (4) have been prepared by reaction of [Fe_4-(OMe)_6(dpm)_6] (5) with tripodal ligands R-C(CH_2OH)_3 (H_3L~1,R = Me;H_3L~2,R = CH_2Br;H_3L~3,R = Ph;H_3L~4,R = ~tBu;Hdpm = dipivaloylmethane).The iron(III) ions exhibit a centered-triangular topology and are linked by six alkoxo bridges,which propagate antiferromagnetic interactions resulting in an S = 5 ground spin state.Single crystals of 4 reproducibly contain at least two geometric isomers.From high-frequency EPR studies,the axial zero-field splitting parameter (D) is invariably negative,as found in 5 (D = -0.21 cm~(-1)) and amounts to -0.445 cm~(-1) in 1,-0.432 cm~(-1) in 2,-0.42 cm~(-1) in 3 centre dot Et_2O,and -0.27 cm~(-1) in 4 (dominant isomer).The anisotropy barrier U_(eff) determined by AC magnetic susceptibility measurements is U_(eff)/k_B = 17.0 K in 1,16.6 K in 2,15.6 K in 3 centre dot Et_2O,5.95 K in 4,and 3.5 K in 5.Both |D| and U_(eff) are found to increase with increasing helical pitch of the Fe(O_2Fe)_3 core.The fourth-order longitudinal anisotropy parameter B_4~O,which affects the shape of the anisotropy barrier,concomitantly changes from positive in 1 ("compressed parabola") to negative in 5 ("stretched parabola").With the aid of spin Hamiltonian calculations the observed trends have been attributed to fine modulation of single-ion anisotropies induced by a change of helical pitch.
机译:具有螺旋桨状结构的Tetrairon(III)单分子磁体(SMM)在高度和形状上均表现出可调节的磁各向异性势垒。簇[Fe_4(L〜1)_2(dpm)_6](1),[Fe_4( L〜2)_2(dpm)_6](2),[Fe4(L〜3)_2(dpm)6]中心点Et_2O(3个中心点Et_2O)和[Fe_4(OEt)_3(L〜4)( dpm)_6](4)是通过[Fe_4-(OMe)_6(dpm)_6](5)与三脚架配体RC(CH_2OH)_3(H_3L〜1,R = Me; H_3L〜2,R = CH_2Br; H_3L〜3,R = Ph; H_3L〜4,R =〜tBu; Hdpm =二戊酰甲烷)。铁(III)离子呈中心三角拓扑并由六个烷氧基桥连接,传播反铁磁相互作用在S = 5的自旋状态。4的单晶可重复包含至少两个几何异构体。根据高频EPR研究,轴向零场分裂参数(D)始终为负,如图5所示(D =- 0.21 cm〜(-1))等于1,-0.445 cm〜(-1)等于2,-0.432 cm〜(-1)2,-3中心点Et_2O等于0.42 cm〜(-1)和-0.27 cm〜(-1)in 4(占主导交流磁化率测量确定的各向异性势垒U_(eff)为U_(eff)/ k_B = 17.0 K in 1,16.6 K in 2,15.6 K in 3中心点Et_2O,5.95 K in 4,和3.5 K在5.Both中| D |发现Fe(O_2Fe)_3芯的螺距增加时,U_(eff)和U_(eff)增大。四阶纵向各向异性参数B_4〜O影响各向异性势垒的形状,其正值从1变为正。压缩抛物线”)到5中的负值(“拉伸抛物线”)。借助自旋哈密顿量计算,观察到的趋势归因于由螺距变化引起的单离子各向异性的精细调制。

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  • 来源
    《Journal of the American Chemical Society》 |2006年第14期|p.4742-4755|共14页
  • 作者单位

    Contribution from the INSTM and Department of Chemistry,University of Modena and Reggio Emilia,via G.Campi 183,41100 Modena,Italy,Laboratoire des Champs Magnetiques Intenses-CNRS,BP166,25 Avenue des Martyrs,38042 Grenoble Cedex 9,France,INSTM and Dep;

    Contribution from the INSTM and Department of Chemistry,University of Modena and Reggio Emilia,via G.Campi 183,41100 Modena,Italy,Laboratoire des Champs Magnetiques Intenses-CNRS,BP166,25 Avenue des Martyrs,38042 Grenoble Cedex 9,France,INSTM and Dep;

    Contribution from the INSTM and Department of Chemistry,University of Modena and Reggio Emilia,via G.Campi 183,41100 Modena,Italy,Laboratoire des Champs Magnetiques Intenses-CNRS,BP166,25 Avenue des Martyrs,38042 Grenoble Cedex 9,France,INSTM and Dep;

    Contribution from the INSTM and Department of Chemistry,University of Modena and Reggio Emilia,via G.Campi 183,41100 Modena,Italy,Laboratoire des Champs Magnetiques Intenses-CNRS,BP166,25 Avenue des Martyrs,38042 Grenoble Cedex 9,France,INSTM and Dep;

    Contribution from the INSTM and Department of Chemistry,University of Modena and Reggio Emilia,via G.Campi 183,41100 Modena,Italy,Laboratoire des Champs Magnetiques Intenses-CNRS,BP166,25 Avenue des Martyrs,38042 Grenoble Cedex 9,France,INSTM and Dep;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 化学;
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