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首页> 外文期刊>Optics and Spectroscopy >Energy transfer between lanthanide ions in nanostructures of their complexes. II
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Energy transfer between lanthanide ions in nanostructures of their complexes. II

机译:镧系元素离子在其配合物的纳米结构中的能量转移。 II

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The changes in the luminescence intensity and in the luminescence lifetime of Eu, Th, and Sm complexes with some beta-diketones and 1,10-phenanthroline that occur upon formation of nanostructures with complexes of triply charged ions Pr, Nd, Sm, Eu, Dy, Ho, Er, Tm, and Yb-acceptors of the electronic excitation of luminescing ions-are compared for the first time. Pairs of lanthanide ions are suggested to exist inside nanostructures, which are bound by a bridge at a distance shorter (0.4 nm) in comparison with the size of interacting complexes. For a large number of pairs of donor and acceptor ions, the averaged probabilities (w(t)) of energy transfer between these ions in nanostructures in the solution of each beta-diketone under study are calculated. Based on the comparison of w(t) with the predictions of the theory of the inductive resonance and exchange resonance energy transfer mechanisms, the average distance R between Ln(III) ions interacting in given fragments of nanostructures is estimated for each donor-acceptor pair, and the energy transfer mechanism is identified for the first time. It is shown that energy can be transferred between Ln(III) ions in nanostructures both according to the inductive resonance and via the exchange resonance mechanisms. The type of the transfer mechanism depends on the spectral parameters of interacting ions and on the ability of complexes of given acceptor ions to form heteronuclear nanostructures, whose composition determines the distance R. The variation in the value of R revealed for different ion pairs is explained by the occurrence of exchange resonance interactions between some ions. The overestimated probabilities w(t) for ion pairs characterized precisely by exchange resonance interactions can be explained by the influence of covalent bonds in nanostructures of Ln chelates on pi conjugation of overlapped electronic shells of interacting particles. By using the method of energy transfer between Ln(III) ions of complexes from distant spheres of a structure, the average minimal size of nanostructures formed is estimated to be 2.6-3.4 nm.
机译:Eu,Th和Sm配合物与一些β-二酮和1,10-菲咯啉的配合物的发光强度和发光寿命的变化是在与三价离子Pr,Nd,Sm,Eu,首次比较了发光离子电子激发的Dy,Ho,Er,Tm和Yb受体。建议在纳米结构内部存在成对的镧系离子,与相互作用的配合物的大小相比,它们在较短的距离(0.4 nm)处被桥键合。对于大量的供体和受体离子对,计算了每个被研究的β-二酮溶液中纳米结构中这些离子之间能量转移的平均概率(w(t))。基于w(t)与感应共振和交换共振能量转移机理理论预测的比较,估计了每个给体-受体对在给定的纳米结构片段中相互作用的Ln(III)离子之间的平均距离R ,并首次确定了能量传递机制。结果表明,能量可以根据感应共振和通过交换共振机制在纳米结构的Ln(III)离子之间转移。转移机制的类型取决于相互作用离子的光谱参数以及给定受体离子的配合物形成异核纳米结构的能力,异核纳米结构的组成决定了距离R。解释了不同离子对的R值变化通过某些离子之间交换共振相互作用的发生。通过交换共振相互作用精确表征的离子对的高估概率w(t)可以通过Ln螯合物纳米结构中的共价键对相互作用粒子的重叠电子壳的π共轭的影响来解释。通过使用能量从结构的远处的球体之间的Ln(III)离子之间转移的方法,形成的纳米结构的平均最小尺寸估计为2.6-3.4 nm。

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