首页> 外文期刊>Vibrational Spectroscopy: An International Journal devoted to Applications of Infrared and Raman Spectroscopy >Raman spectroscopic characteristics of phthalocyanine and naphthlocyanine in sandwich-type phthalocyaninato and porphyrinato rare earth complexes part 4. Raman spectroscopic characterstics of naphthalocyanine in mixed (octaethylporphyrinato) (naphtha
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Raman spectroscopic characteristics of phthalocyanine and naphthlocyanine in sandwich-type phthalocyaninato and porphyrinato rare earth complexes part 4. Raman spectroscopic characterstics of naphthalocyanine in mixed (octaethylporphyrinato) (naphtha

机译:夹心型酞菁和卟啉稀土配合物中酞菁和萘酞菁的拉曼光谱特征第4部分。混合(八乙基卟啉)(石脑油)中萘酞菁的拉曼光谱特征

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Raman spectroscopic data in the range of 400-1800 cm~(-1) for a series of 15 mixed (octaethylporphyrinato)(naphthalocyaninato) double-decker complexes with tervalent rare earths M~(III)(OEP)(2,3-Nc) (M = Y, La,…,Lu except Ce and Pm) and intermediate valent cerium Ce(OEP)(2,3-Nc) have been collected using laser excitation sources emitting at 632.8 and 785 nm. Comparison with the Raman spectra of the corresponding bis(naphthalocyaninato) rare earths reveals that the Raman characteristics of mixed ring double-deckers M(OEP)(2,3-Nc) are dominated by the metallonaphthalocyanine M(2,3-Nc) fragment. Under excitation at 632.8 nm, which is far away from the main Q absorption band of the naphthalocyanine ligand, the most intense Raman band appearsat 1598 cm~(-1) for M~(III) (OEP)(2,3-Nc) (M not= Ce), the is assigned to the naphthalene stretching. On the other hand, for Ce(OEP)(2,3-Nc), this vibration appears as a strongly enhanced peak at 1550 cm~(-1) together with a medium intense band at 1613 cm~(-1). Typical Raman marker bands of the monoanion radical Nc~(·-) were observed at 1499-1512 cm~(-1) as a medium band and at 1512-1538 cm~(-1) as a band whose intensity increases along with the rare earth contraction, resulting from the coupling of pyrrole C = C and aza C = N stretching and aza C = N -only stretchings, respectively. For Ce(OEP)(2,3-Nc), a weak and broad band centered at 1507 cm~(-1) with contribution from both pyrrole C = C and aza C = N stretches together with isoindole stretches was the marker Raman band of Nc~(2-). When excited with laser radiation of 785 nm which is in close resonance with the main Q absorption band of naphthalocyanine ligand, the ring radial vibrations of the isonidole moieties at ca. 680 and 732 cm~(-1) in the Raman spectra of both M~(III)(OEP)(2,3-Nc) and Ce(OEP)(2,3-Nc) are selectively intensified and appear as the most intense vibrations. The marker Raman bands of Nc~(·-) in M~(III)(OEP)(2,3-Nc) and Nc~(2-) in Ce(OEP)(2,3-Nc) are observed in similar regions to those found for excitation at 632.8 nm. The scatterings with contribution from the Nc breathings, ring radial vibration, naphthalene stretchings, benzoisoindole stretchings,aza group stretchings,and the coupling of pyrrole C=C and aza C = N stretchings in M~(III)(OEP)(2,3-Nc) all show dependence on the rare earth radius, shifting to higher energy along with the rare earth contraction and showing the rare earth ionic size effect on the Raman characteristics of naphthalocyanine in the mixed ring double-decker compounds.
机译:15种混合的八价稀土元素M〜(III)(OEP)(2,3-Nc)混合(八乙基卟啉酮)(萘酞菁)双层配合物的拉曼光谱数据在400-1800 cm〜(-1)范围内)(使用Ce和Pm除外的M = Y,La,…,Lu)和中价铈Ce(OEP)(2,3-Nc)已使用在632.8和785 nm处发射的激光激发源进行了收集。与相应的双(萘酞菁钠)稀土元素的拉曼光谱比较表明,混合环双层M(OEP)(2,3-Nc)的拉曼特性主要由金属酞菁M(2,3-Nc)片段决定。在远离萘酞菁配体的主要Q吸收带的632.8 nm激发下,M〜(III)(OEP)(2,3-Nc)的最强拉曼谱带出现在1598 cm〜(-1)处(M not = Ce),将其指定为萘拉伸。另一方面,对于Ce(OEP)(2,3-Nc),该振动在1550 cm〜(-1)处表现为强烈增强的峰,而在1613 cm〜(-1)处表现为中等强度的带。在1499-1512 cm〜(-1)处观察到典型的单阴离子基团Nc〜(·-)的拉曼标记带,在1512-1538 cm〜(-1)处随着强度的增加而增加。分别由吡咯C = C和氮杂C = N拉伸和仅氮杂C = N拉伸耦合引起的稀土收缩。对于Ce(OEP)(2,3-Nc),以吡咯C = C和aza C = N伸展带以及异吲哚伸展带为中心,以1507 cm〜(-1)为中心的弱而宽的带是标记拉曼谱带Nc〜(2-)。当被785 nm的激光辐射激发时,与萘酞菁配体的主Q吸收带紧密共振,异戊二烯部分的环径向振动大约为。 M〜(III)(OEP)(2,3-Nc)和Ce(OEP)(2,3-Nc)的拉曼光谱中的680和732 cm〜(-1)选择性增强并出现最多剧烈震动。类似地观察到M〜(III)(OEP)(2,3-Nc)中Nc〜(·-)和Ce(OEP)(2,3-Nc)中Nc〜(2-)的标记拉曼谱带对于在632.8 nm激发的区域M〜(III)(OEP)(2,3)中Nc呼吸,环径向振动,萘拉伸,苯并异吲哚拉伸,氮杂基团拉伸以及吡咯C = C和氮杂C = N拉伸的耦合作用引起的散射-Nc)都显示出对稀土半径的依赖性,随着稀土的收缩转移到更高的能量,并且显示出稀土离子尺寸大小对混合环双层化合物中萘菁的拉曼特性的影响。

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