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Syntheses, spectroscopic and molecular quadratic nonlinear optical properties of dipolar ruthenium(II) complexes of the ligand 1,2-phenylenebis(dimethylarsine)

机译:配体1,2-亚苯基双(二甲基胂)的偶极钌(II)配合物的合成,光谱和分子二次非线性光学性质

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摘要

Six new complex salts trans-[RuIICl(pdma)2L][PF 6]n [pdma = 1,2-phenylenebis(dimethylarsine); L = (E,E,E)-1,6-bis(4-pyridyl)hexa-1,3,5-triene (bph), n = 1,5; L = N-methyl-4-[(e)-2-(4-pyridyl)ethenyl]pyridinmm (Mebpe-), n = 2, 7; L = N-methyl-4-[(E,E)-4-(4-pyridyl)buta-1,3-dienyl]pyridinium (Mebpb+), n = 2, 8; L = N-methyl-4-{(E,E,E)-6-(4-pyridyl)hexa1,3,5-trienyl}pyridinium (Mebph+), n = 2,9; L = bis(4-pyridyl)acetylene (bpa), n = 1, 10; L = N-methyl-4-[2-(4-pyridyl)-ethynyl]pyridinium (Mebph+), n = 2, 11] have been prepared. The electronic absorption spectra of 5 and 7-11 display intense, visible metal-to-ligand charge-transfer (MLCT) bands, with λmax values in the range 434-492 nm in acetonitrile. Cyclic voltammetric studies reveal reversible RuIII/II waves with E1/2 values in the range 1.06-1.15 V vs. Ag-AgCl, Natogether with irreversible L-based reduction processes. Along with a number of previously reported related compounds (B. J. Coe et al., J. Chem. Soc., Dalton Trans., 1996, 3917; 1997, 591; 2000, 797), salts 5 and 7-11 have been investigated by using Stark (electroabsorption) spectroscopy in butyronitrile glasses at 77 K. These studies have afforded dipole moment changes Δμ12 for the MLCT transitions which have been used to calculate molecular static first hyperpolarizabilities β0 according to the two-state equation β0 = 3Δμ12(μ12) 2/(Emax)2(μ12= transition dipole moment, Emax = MLCT energy). MLCT absorption and electrochemical data show that a trans-{RuIICl(pdma)2}+ centre is considerably less electron-rich than a {RuII(NH3) 5}2- unit. Although the β0 responses of the pdma complexes are only a little smaller than those of their {Ru II(NH3)5}2- analogues, this result is partly attributable to unexpected changes in the relative π12 values on freezing. Thus, substantial increases in μ12 for the arsine compounds act to partially offset the β0-decreasing influence of their higher Emax values when compared with the analogous pentaammine species. Single crystal X-ray structures have been obtained for the salts 1-2.5MeCN, 4·2MeCN, 7 and 11, but only 1-2.5MeCN adopts a non-centrosymmetric space group (Fdd2) such as may show bulk NLO effects.
机译:六种新的复合盐反式-[RuIICl(pdma)2L] [PF 6] n [pdma = 1,2-亚苯基双(二甲基ar); L =(E,E,E)-1,6-双(4-吡啶基)己-1,3,5-三烯(bph),n = 1,5; L = N-甲基-4-[(e)-2-(4-吡啶基)乙烯基]吡啶鎓mm(Mebpe-),​​n = 2、7; L = N-甲基-4-[(E,E)-4-(4-吡啶基)丁-1,3-二烯基]吡啶鎓(Mebpb +),n = 2,8; L = N-甲基-4-{(E,E,E)-6-(4-吡啶基)六,3,5-三烯基}吡啶鎓(Mebph +),n = 2.9; L =双(4-吡啶基)乙炔(bpa),n = 1,10;已经制备了L = N-甲基-4- [2-(4-吡啶基)-乙炔基]吡啶鎓(Mebph +),n = 2、11]。 5和7-11的电子吸收光谱显示出强烈的可见金属-配体电荷转移(MLCT)谱带,乙腈中的λmax值在434-492 nm范围内。循环伏安法研究显示,与Ag-AgCl相比,E1 / 2值在1.06-1.15 V范围内的可逆RuIII / II波,以及不可逆的基于L的还原过程。连同许多先前报道的相关化合物(BJ Coe等人,J. Chem。Soc。,Dalton Trans。,1996,3917; 1997,591; 2000,797),盐5和7-11的研究已经通过使用Stark(电吸收)光谱在77 K的丁腈玻璃中进行。这些研究提供了MLCT跃迁的偶极矩变化Δμ12,该跃迁已用于根据二态方程β0=3Δμ12(μ12)2来计算分子静态第一超极化率β0。 /(Emax)2(μ12=跃迁偶极矩,Emax = MLCT能量)。 MLCT吸收和电化学数据表明,反式{RuIICl(pdma)2} +中心的电子富集度比{RuII(NH3)5} 2-单元小得多。尽管pdma配合物的β0响应仅比其{Ru II(NH3)5} 2-类似物的响应小一些,但该结果部分归因于冻结时相对π12值的意外变化。因此,与类似的五胺类物质相比,rs化合物的μ12大幅增加可部分抵消其较高Emax值的β0降低影响。已经获得了盐1-2.5MeCN,4·2MeCN,7和11的单晶X射线结构,但是只有1-2.5MeCN采用非中心对称的空间基团(Fdd2),例如可能显示出大量的NLO效应。

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