首页> 外文OA文献 >A Series of Tetrathiafulvalene-Based Lanthanide Complexes Displaying Either Single Molecule Magnet or Luminescence-Direct Magnetic and Photo-Physical Correlations in the Ytterbium Analogue
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A Series of Tetrathiafulvalene-Based Lanthanide Complexes Displaying Either Single Molecule Magnet or Luminescence-Direct Magnetic and Photo-Physical Correlations in the Ytterbium Analogue

机译:一系列四硫富瓦烯基镧系配合物,在镱类似物中显示单分子磁体或发光直接磁性和光物理相关性

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摘要

The reaction between (4,5-bis(2-pyridyl-N-oxidemethylthio)-4,5)-ethylenedithiotetrathiafulvene (L-1) or -methyldithiotetrathiafulvene (L-2) ligands and Ln(hfac)(3)center dot nH(2)O precursors (Ln(III) = Pr, Tb, Dy, Er, and Yb) leads to the formation of seven dinudear complexes of formula [Ln(2)(hfac)(6)(H2O)(x)(L-y)(2)] (x = 2 and y = 1 for L-III = Pr (1); x = 0 and y = 1 for Ln(III) = Tb (2), Dy (3), Er (4) and Yb (5); x = 0 and y = 2 for Ln(III) = Tb (6) and Dy (7)). Their X-ray structures reveal that the coordination environment of each Ln(III) center is filled by two N-oxide groups coming from two different ligands L-y. UV-visible absorption properties have been experimentally measured and rationalized by TD-DFT calculations. The temperature dependences of static magnetic measurements have been fitted. The ground state corresponds to the almost pure vertical bar M-J = +/- 13/2 while the first excited state (+/- 0.77 vertical bar +/- 11/2 +/- 0.50 vertical bar +/- 3/2 +/- 0.39 vertical bar +/- 5/2) is located at 19 cm(-1) and 26.9 cm(-1) respectively for 3 and 7. Upon irradiation at 77 K and at room temperature, in the range 25 000-20 835 cm(-1), both compounds 4 and 5 display a metal-centered luminescence attributed to I-4(13/2) -I-4(15/2) (6660 cm(-1)) and F-2(5/2) -E-2(7/2) (9972 cm(-1)) transitions, respectively. Emission spectroscopy provides a direct probe of the vertical bar +/- 5/2 ground state multiplet splitting, which has been confronted to magnetic data. The energy separation of 225 cm(-1) between the ground state and the first excited level (M-J = +/- 3/2) fits exactly the second emission line (234 cm(-1)). While no out-phase-signal is detected for 3, the change of ligand L-1 - L-2 induces a change of coordination sphere symmetry around the Dy-III increasing the energy splitting between the ground and first excited states, and 7 displays a single molecule magnet behavior.
机译:(4,5-双(2-吡啶基-N-氧化物甲硫基)-4,5)-乙撑二硫代四硫富烯(L-2)配体与Ln(hfac)(3)中心点nH的反应(2)O前体(Ln(III)= Pr,Tb,Dy,Er和Yb)导致形成七个式[Ln(2)(hfac)(6)(H2O)(x)( Ly)(2)](对于L-III = Pr(1),x = 2,y = 1;对于Ln(III)= Tb(2),Dy(3),Er(4,x = 0,y = 1 )和Yb(5);对于Ln(III)= Tb(6)和Dy(7)),x = 0,y = 2。它们的X射线结构表明,每个Ln(III)中心的配位环境都被来自两个不同配体L-y的两个N-氧化物基团填充。通过TD-DFT计算对紫外线可见吸收特性进行了实验测量和合理化。静态磁测量的温度依赖性已得到拟合。基态对应于几乎纯的垂直线MJ = +/- 13/2,而第一激发态(+/- 0.77垂直线+/- 11/2 +/- 0.50垂直线+/- 3/2 + / -0.39垂直条(+/- 5/2)分别位于3和7的19 cm(-1)和26.9 cm(-1)处。在77 K和室温下照射时,范围为25000-20 835 cm(-1),化合物4和5均显示归因于I-4(13/2)-I-4(15/2)(6660 cm(-1))和F-2( 5/2)-E-2(7/2)(9972 cm(-1))过渡。发射光谱法提供了垂直棒+/- 5/2基态多重态分裂的直接探测,这已经遇到了磁性数据。基态与第一激发能级(M-J = +/- 3/2)之间的225 cm(-1)能量间隔正好适合第二发射线(234 cm(-1))。虽然没有检测到3的异相信号,但配体L-1-L-2的变化引起了Dy-III周围配位球对称性的变化,从而增加了基态和第一激发态之间的能量分配,并且显示7单分子磁体的行为。

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