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[Pt{4'-(R)三联吡啶}(CN)]⁺(R = 苯基、邻甲基苯基、邻氯苯基或邻三氟甲基苯基;三联吡啶 = 2,2':6',2''-三联吡啶)的合成、电化学性质及发光特性:[Pt{4'-(苯基)三联吡啶}(CN)]BF₄·CH₃CN的晶体结构

Synthesis, electrochemistry and luminescence of [Pt{4'-(R)trpy}(CN)](+) (R = Ph, o-CH(3)C(6)H(4), o-ClC(6)H(4) or o-CF(3)C(6)H(4); trpy = 2,2':6',2''-terpyridine): crystal structure of [Pt{4'-(Ph)trpy}(CN)]BF(4) x CH(3)CN.

作者信息

Field John S, Haines Raymond J, Ledwaba Lesibana P, McGuire Robert, Munro Orde Q, Low Murray R, McMillin David R

机构信息

School of Chemistry, University of KwaZulu-Natal, Private Bag X01, Pietermaritzburg, 3201, South Africa.

出版信息

Dalton Trans. 2007 Jan 14(2):192-9. doi: 10.1039/b611244g. Epub 2006 Nov 16.

Abstract

The synthesis and characterization of [Pt{4'-(R)trpy}(CN)]X (R = Ph, X = BF(4) or SbF(6); R = o-CH(3)C(6)H(4), X = SbF(6); R = o-ClC(6)H(4), X = SbF(6); or R = o-CF(3)C(6)H(4), X = SbF(6)) are described where trpy = 2,2':6',2''-terpyridine. Single crystals of [Pt{4'-(Ph)trpy}(CN)]BF(4).CH(3)CN were grown by vapour diffusion of diethyl ether into an acetonitrile solution of [Pt{4'-(Ph)trpy}(CN)]BF(4). An X-ray crystal structure determination of the solvated complex confirms the near linear coordination of the cyanide ligand to the platinum centre. The cation is almost planar as evidenced by a twist of only 1.9 degrees of the phenyl group out of the plane of the terpyridyl moiety. Cyclic voltammograms were recorded in DMF/0.1 M TBAH for the Pt{4'-(R)trpy}(CN) cations. Two quasi-reversible one-electron reduction (cathodic) waves are observed with E(1/2) values that show the trend expected for an increasingly lower energy of the trpy-based LUMO of the complex i.e., Pt{4'-(Ph)trpy}(CN) approximately Pt{4'-(o-CH(3)C(6)H(4))trpy}(CN) < Pt{4'-(o-ClC(6)H(4))trpy}(CN) < Pt{4'-(o-CF(3)C(6)H(4))trpy}(CN). All the Pt(4'-(R)trpy}(CN) cations are photoluminescent in dichloromethane. Emission by Pt{4'-(Ph)trpy}(CN) is from an excited state with largely (3)MLCT orbital parentage, but with some intraligand (3)pi-pi* character mixed-in (tau = 0.1 micros). In contrast, the other three cations display emission that appears exclusively intraligand (3)pi-pi* in origin (tau approximately 0.8 micros). Emission spectra have been recorded in a low concentration frozen DME {1 : 5 : 5 (v/v) DMF-MeOH-EtOH} glass. For the R = o-CH(3)C(6)H(4), o-ClC(6)H(4) and o-CF(3)C(6)H(4) cations the envelope of vibronic structure and energies of the vibrational components are essentially the same as that recorded in dichloromethane. However, for the Pt{4'-(Ph)trpy}(CN) cation, there is a blue-shift in the energies of the vibrational components as compared to that recorded in dichloromethane, as well as a change in the envelope of vibronic structure to a more "domed" pattern; this has been interpreted in terms of a higher percentage of intraligand (3)pi-pi* character in the emitting state for the glass. Increasing the concentration of the glass invariably leads to aggregation of the cations and the consequent development of new low energy bands, such that at 0.200 mM broad peaks centred at ca. 650 and 700 nm dominate the spectrum; these bands are assigned to excimeric (3)pi-pi* and (3)MMLCT emission, respectively.

摘要

描述了[Pt{4'-(R)trpy}(CN)]X(R = Ph,X = BF₄或SbF₆;R = o-CH₃C₆H₄,X = SbF₆;R = o-ClC₆H₄,X = SbF₆;或R = o-CF₃C₆H₄,X = SbF₆)的合成与表征,其中trpy = 2,2':6',2''-三联吡啶。通过将乙醚蒸汽扩散到[Pt{4'-(Ph)trpy}(CN)]BF₄的乙腈溶液中,生长出了[Pt{4'-(Ph)trpy}(CN)]BF₄·CH₃CN的单晶。对溶剂化配合物的X射线晶体结构测定证实了氰化物配体与铂中心的近线性配位。阳离子几乎是平面的,苯基仅从三联吡啶部分的平面扭转1.9度就证明了这一点。在DMF/0.1 M TBAH中记录了[Pt{4'-(R)trpy}(CN)]⁺阳离子的循环伏安图。观察到两个准可逆的单电子还原(阴极)波,其E₁/₂值显示出该配合物基于三联吡啶的最低未占分子轨道(LUMO)能量越来越低的预期趋势,即[Pt{4'-(Ph)trpy}(CN)]⁺≈[Pt{4'-(o-CH₃C₆H₄)trpy}(CN)]⁺<[Pt{4'-(o-ClC₆H₄)trpy}(CN)]⁺<[Pt{4'-(o-CF₃C₆H₄)trpy}(CN)]⁺。所有的[Pt(4'-(R)trpy}(CN)]⁺阳离子在二氯甲烷中都有光致发光现象。[Pt{4'-(Ph)trpy}(CN)]⁺的发射来自一个主要具有(³)MLCT轨道性质,但混入了一些配体内(³)π-π性质的激发态(τ = 0.1微秒)。相比之下,其他三种阳离子的发射似乎完全源于配体内(³)π-π(τ约为0.8微秒)。在低浓度冷冻的DME{1 : 5 : 5(v/v)DMF - 甲醇 - 乙醇}玻璃中记录了发射光谱。对于R = o-CH₃C₆H₄、o-ClC₆H₄和o-CF₃C₆H₄阳离子,振动结构的包络和振动成分的能量与在二氯甲烷中记录的基本相同。然而,对于[Pt{4'-(Ph)trpy}(CN)]⁺阳离子,与在二氯甲烷中记录的相比,振动成分的能量发生了蓝移,并且振动结构的包络变为更“圆顶状”的模式;这被解释为玻璃发射态中配体内(³)π-π性质的百分比更高。增加玻璃的浓度总是会导致阳离子聚集,并随之产生新的低能量带,使得在0.200 mM时,以约650和700 nm为中心的宽峰主导光谱;这些带分别被指定为准分子(³)π-π和(³)MMLCT发射。

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