首页> 外文期刊>Inorganica Chimica Acta >LIGAND-CENTERED (3)PI-PI-ASTERISK EMISSION AND RAMAN ACTIVITY OF [PT(BPY-H(8))(N)(BPY-D(8))(2-N)](2T) (N=O, 1, 2)
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LIGAND-CENTERED (3)PI-PI-ASTERISK EMISSION AND RAMAN ACTIVITY OF [PT(BPY-H(8))(N)(BPY-D(8))(2-N)](2T) (N=O, 1, 2)

机译:[PT(BPY-H(8))(N)(BPY-D(8))(2-N)](2T)的配体定心(3)PI-PI-星形发射和拉曼活性(N = O ,1,2)

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Highly resolved emission and excitation spectra as well as emission decay data of [Pt(bpy-h(8))(n)(bpy-d(8))(2-n)](2+) (n = 0, 1, 2;bpy = 2,2'-bipyridine) are presented. These compounds are investigated as traps in neat [Pt(bpy)(2)](ClO4)(2) matrices. The traps, having their emitting states several cm(-1) below those of the majority of complexes, lead to spectral resolutions, which are by a factor of several hundreds better than hitherto published. The highest resolution of approximate to 4 cm(-1) is found for [Pt(bpy-h(8))(2)](2+) doped into [Pt(bpy-d(8))(2)](ClO4)(2). The low-lying electronic origins (0-0 lines), e.g. at 21 237 cm(-1) for [Pt(bpy-h(8))(2)](2+) in [Pt(bpy-h(8))(2)] (ClO4)(2), and the well-resolved vibrational satellite structures carry the information needed for a classification of the lowest electronic states. They are assigned as ligand centered of of (3) pi pi* character with small metal admixtures. The partially deuterated [Pt(bpy-h(8)) (bpy-d(8))](2+) emits only from the energetically lower lying (bpy-h(8))-ligand due to an effective intra-molecular energy transfer, which quenches the emission from the (bpy-d(8))-ligand and prevents a dual emission. The spectra reveal further that a significant vibrational ligand-ligand coupling of (high-energy) internal ligand modes does not take place. Raman spectra of the neat perchlorate materials are also presented. In particular, the Raman spectrum of [Pt(bpy-h(8)) (bpy-d(8))](2+) consists of a superposition of (bpy-h(8))- and (bpy-d(8))-ligand modes. Interestingly, the (bpy-d(8))-ligand exhibits much higher Raman scattering intensities than the (bpy-h(8))-ligand. An important message is found from the comparison of the emission with the Raman spectrum of [Pt(bpy-h(8)) (bpy-d(8))](2+). This comparison demonstrates the different kinds of information carried by the two types of spectra. Raman lines are observed for both ligands, while the emission spectrum is highly selective and displays just the information about the spatial region of the complex, which is responsible for the electronic transition. (C) 1997 Elsevier Science S.A. [References: 66]
机译:[Pt(bpy-h(8))(n)(bpy-d(8))(2-n)](2+)的高分辨率解析发射和激发光谱以及发射衰减数据(n = 0,1 ,2; bpy = 2,2′-联吡啶。这些化合物被作为纯[Pt(bpy)(2)](ClO4)(2)基质中的陷阱进行了研究。陷阱的发射态比大多数络合物的发射态低几厘米(-1),从而导致光谱分辨率高出迄今为止公布的几百倍。对于[Pt(bpy-h(8))(2)](2+)掺杂到[Pt(bpy-d(8))(2)](中,发现了大约4 cm(-1)的最高分辨率ClO4)(2)。地势较低的电子起源(0-0行),例如在[Pt(bpy-h(8))(2)](ClO4)(2)中的[Pt(bpy-h(8))(2)](2+)在21237 cm(-1)处,以及分辨率很好的振动卫星结构携带了对最低电子状态进行分类所需的信息。它们被指定为以(3)pi pi *特征与小金属混合物为中心的配体。由于有效的分子内作用,部分氘化的[Pt(bpy-h(8))(bpy-d(8))](2+)仅从能量较低的(bpy-h(8))配体发射能量转移,可抑制(bpy-d(8))配体的发射并防止双重发射。光谱进一步揭示了(高能)内部配体模式没有发生明显的振动配体-配体偶联。还显示了纯高氯酸盐材料的拉曼光谱。特别地,[Pt(bpy-h(8))(bpy-d(8))](2+)的拉曼光谱由(bpy-h(8))-和(bpy-d( 8))-配体模式。有趣的是,(bpy-d(8))-配体比(bpy-h(8))-配体表现出更高的拉曼散射强度。从发射与[Pt(bpy-h(8))(bpy-d(8))](2+)的拉曼光谱的比较中发现了一个重要的信息。这种比较说明了两种光谱所携带的不同类型的信息。对于两个配体都观察到拉曼线,而发射光谱具有高度选择性,并且仅显示有关配合物空间区域的信息,该信息负责电子跃迁。 (C)1997 Elsevier Science S.A. [参考:66]

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