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[Pt(2,2':6',2''-terpyridine)Cl]SbF6 | 195533-29-0

中文名称
——
中文别名
——
英文名称
[Pt(2,2':6',2''-terpyridine)Cl]SbF6
英文别名
[platinum(II)(chloride)(2,2':6',2''-terpyridine)](hexafluoroantimonate(V));[Pt(2,2':6',2''-terpyridine)Cl][SbF6];[Pt(trpy)Cl][SbF6];[PtCl(tpy)](SbF6)
[Pt(2,2':6',2''-terpyridine)Cl]SbF6化学式
CAS
195533-29-0
化学式
C15H11ClN3Pt*F6Sb
mdl
——
分子量
699.546
InChiKey
KQXJTORUQGCIAV-UHFFFAOYSA-G
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    None
  • 重原子数:
    None
  • 可旋转键数:
    None
  • 环数:
    None
  • sp3杂化的碳原子比例:
    None
  • 拓扑面积:
    None
  • 氢给体数:
    None
  • 氢受体数:
    None

反应信息

  • 作为反应物:
    描述:
    [Pt(2,2':6',2''-terpyridine)Cl]SbF6silver thiocyanate乙腈 为溶剂, 以62%的产率得到[Pt(2,2':6',2''-terpyridine)(NCS)]SbF6
    参考文献:
    名称:
    [Pt(trpy)(NCS)] SbF 6的溶液形态,固态光谱和气相致变色,其中trpy = 2,2':6',2''-叔吡啶†
    摘要:
    [Pt(trpy)Cl] SbF 6的处理氯化银在复分解反应中,经过处理后得到[Pt(trpy)(NCS)] SbF 6 ·CH 3 CN的黄色晶体,其中trpy为2,2':6',2''-吡啶。单晶结构测定的溶剂化物显示,SCN -离子是ñ-结合到Pt原子上,并且平面阳离子堆叠为 铂2Pt⋯Pt间距为3.293(1)Å的二聚体。晶体在环境条件下迅速去溶剂化,得到表征为[Pt(trpy)(NCS)] SbF 6(1)的多晶褐红色材料。甲15同位素标记的溶液[铂(trpy)(N的NMR光谱研究15 Ñ 13 CS)]的SbF 6在CD 3 CN表明SCN的两个联动异构体-离子共存与溶液N-结合异构体占主导地位,与S结合的异构体的浓度要低得多。化合物1表现出温度依赖性3固态MMLCT发射; 在280 k中的发射最大化在692纳米,但红移系统上冷却至达到762纳米,在80 K.化合物1示出vapo
    DOI:
    10.1039/b916897b
  • 作为产物:
    参考文献:
    名称:
    Metal–metal stacking patterns between and with [Pt(tpy)X]+ cations
    摘要:
    A comparative study of metallophilic interactions of [Pt(tpy)X](+) cations (tpy = 2,2': 6',2 ''-terpyridine) in the presence of two different types of anions, (i) [AuX2'] anions that form double salts and (ii) simple p-block anions, is reported. Single-crystal X-ray diffraction data, solution-state Pt-195 NMR spectra, and variable temperature solid-state luminescence spectra are reported. Three [Pt(tpy)Cl]Y derivatives (Y = SbF6, 1, SbF6 center dot CH3CN, 4, PF6, 2) and the [Pt(tpy)Br]PF6 analog, 3, as well as two new double salts [Pt(tpy)CN][Au(CN)(2)], 5, and [Pt(tpy)CN](2)[Au(C6F5)(2)](PF6), 6, have been synthesized and characterized. Structural analysis shows consistent patterns in Pt center dot center dot center dot Pt interactions that vary slightly depending on the coordinating halogen or pseudo-halogen X, counter anion Y, and lattice solvent. Metallophilic interactions are seen between [Pt(tpy)X](+) cations with all types of X ligands, but only with pi-accepting X' ligands from [AuX2'] anions are Pt center dot center dot center dot Au metallophilic interactions seen to be favored over Pt center dot center dot center dot Pt interactions. The [Au(CN)(2)] anion consistently forms Pt center dot center dot center dot Au metallophilic contacts, unlike [Au(C6F5)(2)] . The Pt-195 NMR chemical shifts are similar to-2750 ppm for pi-donor ligands and near -3120 ppm for pi-acceptor ligands in [Pt(tpy)X]PF6 compounds. Luminescence data show an unusual blue shift in [Pt(tpy)CCPh][Au(C6F5)(2)] versus [Pt(tpy)CCPh]PF6 ascribed to an intermolecular charge transfer. (C) 2010 Elsevier B.V. All rights reserved.
    DOI:
    10.1016/j.ica.2010.07.038
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文献信息

  • Luminescence Properties of Salts of the [Pt(trpy)Cl]<sup>+</sup> and [Pt(trpy)(MeCN)]<sup>2+</sup> Chromophores:  Crystal Structure of [Pt(trpy)(MeCN)](SbF<sub>6</sub>)<sub>2</sub>
    作者:Riaan Büchner、John S. Field、Raymond J. Haines、Corey T. Cunningham、David R. McMillin
    DOI:10.1021/ic961068b
    日期:1997.8.1
    The crystal structure of [Pt(trpy)(MeCN)](SbF6)(2), where trpy denotes 2,2':6',2 ''-terpyridine, shows that the platinum complex packs as a monomer; however, the (3) pi-pi emission of the solid occur at surprisingly long wavelengths at room temperature. At lower temperatures new, shorter-wavelength maxima appear. Of the known sails with the composition [Pt(trpy)Cl]A, the A = SbF6- system is the lone example that exhibits a temperature-independent emission maximum. In these platinum(II) terpyridines, energy migration to defects or trap sites is one of the phenomena responsible for the temperature dependence of the solid-state emission spectrum. IT trap emission is evident, the low-temperature spectral data are most representative of the bulk material.
  • Synthesis, crystal structure and solid state photoluminescence of [Pt(trpy)(CCPh)]SbF6 (trpy=2,2′:6′,2″-terpyridine)
    作者:Riaan Büchner、John S. Field、Raymond J. Haines、Lesibana P. Ledwaba、Robert McGuire、David R. McMillin、Orde Q. Munro
    DOI:10.1016/j.ica.2006.08.061
    日期:2007.4
    The synthesis a and characterisation of an orange polymorph of [Pt(trpy)(C CPh)]SbF6 is described where trpy = 2,2':6',2 ''-terpyridine. An X-ray crystal structure determination at 293 K reveals that the cations are planar and stacked head-to-tail with alternating Pt center dot center dot center dot Pt distances of 3.604(l) and 4.412(l) angstrom. The perpendicular distances between successive cation planes are constant along the stack at a value of 3.33 angstrom. Crystal structure determinations at 240 and 200 K show that reducing the temperature to 200 K has no significant effect on the cation arrangement, However, below 200 K there is a phase change that we have not been able to characterise, but which has an effect on the solid state photoluminescence exhibited by [Pt(trpy)(C CPh)]SbF6. Thus, whereas at temperatures of >= 200 K, a broad peak with two components at ca. 566 and 597 nm is observed, below 200 K a longer wavelength peak develops that red-shifts as the temperature is lowered [lambda(em)(max) = 637 nm at 80 K]. We assign the >= 200 K emission as (MLLCT)-M-3 in origin, since the X-ray data show that ligand-ligand (LL) and not metal metal (MM) interactions are important at T >= 200 K. On the other hand, the long wavelength emission observed below 200 K is typical of (MMLCT)-M-3 emission, suggesting that the phase change leads to d(z2) (Pt)-d(z2) (Pt) orbital interactions. Of particular interest is that the cation exhibits (MLCT)-M-3 emission in dichloromethane that maximizes at 619 nm, i.e., the high temperature solid state emission occurs at a shorter wavelength, an unexpected result since intermolecular interactions in the solid usually cause the emission to occur at longer wavelengths. A possible explanation for this unexpected result is given. (c) 2006 Elsevier B.V. All rights reserved.
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