Yam Vivian Wing-Wah, Tang Rowena Pui-Ling, Wong Keith Man-Chung, Lu Xiao-Xia, Cheung Kung-Kai, Zhu Nianyong
Department of Chemistry, HKU-CAS Joint Laboratory of New Materials, The University of Hong Kong, SAR, People's Republic of China.
Chemistry. 2002 Sep 2;8(17):4066-76. doi: 10.1002/1521-3765(20020902)8:17<4066::AID-CHEM4066>3.0.CO;2-O.
A series of platinum (II) C empty set N empty set C complexes, [Pt(C empty set N empty set C) (L)] (HC empty set N empty set CH=2,6-diphenylpyridine (dppy); L=Ph(2)PB15C5 (1, B15C5=benzo[15]crown-5), Ph(2)PDMP (2, DMP=3,4-dimethoxyphenyl), pyCOA15C5 (3, A15C5=aza[15]crown-5), pyCON(CH(2)CH(2)OCH(3))(2) (4), pyC[triple bond]CB15C5 (5), pyC[triple bond]CDMP (6)) and terpyridyl complexes, Pt(trpy)(L)(2) (trpy=2,2':6',2''-terpyridine; L=Ph(2)PB15C5, X=OTf (7 a), PF(6) (7 b); X=PF(6), L=Ph(2)PDMP (8), pyC[triple bond]CB15C5 (9), and pyC[triple bond]CDMP (10)) have been successfully synthesized and characterized. The structures of 1, 3, and 7 a have been determined by X-ray crystallography. Excitation of complexes 1-6 in EtOH/MeOH (4:1 v/v) glass gave high-energy structured emission bands, assigned as derived from states of metal-perturbed intraligand (IL) origin. At higher concentrations, complexes 3-6 each displayed an additional, structureless emission band at 600-615 nm, with complexes 5 and 6 showing an obvious increase in the intensity of this emission band when the concentration was increased further. In dichloromethane at room temperature, complexes 3-6 showed, in addition to the high-energy emission at 490-505 nm, an extra, broad emission band at 620-625 nm when the concentration was increased. The emission origins of the low-energy band in glass and in fluid solutions are suggested to be derived from the ground-state oligomerization or aggregation process of the complexes. In the solid state at room temperature, complexes 1-6 each showed a broad, unstructured emission band at 560-600 nm, which was shifted to lower energy upon cooling to 77 K. On the other hand, the terpyridyl analogues 7-10 displayed intense vibronic-structured intraligand (IL) emissions at 460-472 nm in butyronitrile glass at 77 K. Solid-state samples of 9 and 10 displayed strong phosphorescence upon photoexcitation at 298 K and 77 K, tentatively assigned as derived from states of Pt(d pi)-->pi*(trpy) (3)MLCT origin(MLCT=metal-to-ligand charge transfer). The ion-binding properties of complexes 5 and 9 for Na(+), Ba(2+), and K(+) ions have been studied by UV/Vis spectrophotometric methods, and confirmed by ESI mass spectrometric studies. The ion-binding properties for Na(+) ions have also been probed by (1)H NMR experiments. For the same crown ether-containing ligand and the same metal ions, the neutral cyclometalated complexes gave larger binding constants than the positively charged terpyridyl analogues.
一系列铂(II)C≡N≡C配合物,[Pt(C≡N≡C)(L)](HC≡N≡CH = 2,6 - 二苯基吡啶(dppy);L = Ph₂PB15C5(1,B15C5 = 苯并[15]冠 - 5),Ph₂PDMP(2,DMP = 3,4 - 二甲氧基苯基),pyCOA15C5(3,A15C5 = 氮杂[15]冠 - 5),pyCON(CH₂CH₂OCH₃)₂(4),pyC≡CB15C5(5),pyC≡CDMP(6))和三联吡啶配合物,Pt(trpy)(L)₂(trpy = 2,2':6',2'' - 三联吡啶;L = Ph₂PB15C5,X = OTf(7a),PF₆(7b);X = PF₆,L = Ph₂PDMP(8),pyC≡CB15C5(9),和pyC≡CDMP(10))已成功合成并表征。1、3和7a的结构已通过X射线晶体学确定。在乙醇/甲醇(4:1 v/v)玻璃中对配合物1 - 6进行激发,得到高能结构化发射带,归因于金属扰动的配体内(IL)态。在较高浓度下,配合物3 - 6在600 - 615 nm处各自显示出一个额外的无结构发射带,当浓度进一步增加时,配合物5和6的该发射带强度明显增加。在室温下的二氯甲烷中,当浓度增加时,配合物3 - 6除了在490 - 505 nm处有高能发射外,在620 - 625 nm处还显示出一个额外的宽发射带。玻璃态和流体溶液中低能带的发射起源被认为源自配合物的基态低聚或聚集过程。在室温下的固态中,配合物1 - 6各自在560 - 600 nm处显示出一个宽的无结构发射带,冷却至77 K时该发射带向低能量移动。另一方面,三联吡啶类似物7 - 10在77 K的丁腈玻璃中在460 - 472 nm处显示出强烈的振动结构配体内(IL)发射。9和10的固态样品在298 K和77 K光激发时显示出强磷光,初步归因于Pt(dπ)→π*(trpy)(³MLCT)态(MLCT = 金属到配体的电荷转移)。通过紫外/可见分光光度法研究了配合物5和9对Na⁺、Ba²⁺和K⁺离子的离子结合性质,并通过电喷雾质谱研究得到证实。还通过¹H NMR实验探测了对Na⁺离子的离子结合性质。对于相同的含冠醚配体和相同的金属离子,中性环金属化配合物给出的结合常数比带正电荷的三联吡啶类似物大。