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New contributions to the photophysical model for all-trans-polyenes from ttbP4, a nonphotolabile octatetraene

机译:ttbP4(一种非光不稳定的辛酸酯)对全反式多烯的光物理模型的新贡献

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All-trans-octatetraene 3,10-di(tert-butyl)-2,2,11,11-tetramethyl-3,5,7,9-dodecatetraene emits fluorescence in three different regions of the visible spectrum. Thus, it produces an extremely weak emission in the gas phase that can hardly be detected in the condensed phase; such an emission exhibits a negligible Stokes shift with respect to the 1A(g)-> 1B(u) absorption transition and can, in principle, be assigned to the 1B(u)-> 1A(g) emission for the compound. A second, structureless fluorescence emission, centered in the region of 525 nm, is observed in the gas phase and at somewhat higher wavelengths in the condensed phase [viz., 570 nm in 2-methylbutane (2MB) and 550 nm in squalane (SQ)]. While detectable, this emission increases significantly, with no change in spectral position, as the solution temperature is lowered; also, it is abruptly replaced by a new, strongly blueshifted emission at similar to 490 nm in 2MB and 455 mm in SQ when the viscosity of the medium exceeds a given level. The fact that the two fluorescence emissions considerably depart from the expected behavior for a 1B(u)-> 1A(g) emission in an all-trans-polyene, and that one disappears while the other simultaneously appears as the medium becomes more rigid, suggests that the two emissions are produced by two different molecular structures and that the rigidity of the medium switches their production from the originally excited all-trans 1B(u) form. The observed spectral behavior is consistent with a recently proposed model [J. Catalan, Chem. Phys. 335, 69 (2007)] in which the 1B(u) excited state of octatetraene can give two distinct molecular conformers as a result of twisting about different C-C single bonds. (c) 2008 American Institute of Physics.
机译:全反式辛酸酯3,10-二(叔丁基)-2,2,11,11-四甲基-3,5,7,9-十二碳烯在可见光谱的三个不同区域中发出荧光。因此,它在气相中产生极弱的发射,在冷凝相中几乎检测不到。这样的发射相对于1A(g)-> 1B(u)吸收跃迁表现出微不足道的斯托克斯位移,并且原则上可以归为化合物的1B(u)-> 1A(g)发射。在气相中观察到第二个无结构荧光发射,中心在525 nm范围内,在冷凝相中观察到更高的波长[即2-甲基丁烷(2MB)为570 nm,角鲨烷(SQ为550 nm) )]。虽然可以检测到,但是随着溶液温度的降低,这种发射显着增加,而光谱位置没有变化。同样,当介质的粘度超过给定水平时,它会突然被新的强烈蓝移发射所替代,该发射在2MB中接近490 nm,在SQ中接近455 mm。在全反式多烯中,两种荧光发射都大大偏离了1B(u)-> 1A(g)发射的预期行为,并且当介质变得更硬时,一种消失,而另一种同时出现,这表明这两种发射是由两种不同的分子结构产生的,并且介质的刚度从最初激发的全反式1B(u)形式切换了它们的产生。观察到的光谱行为与最近提出的模型是一致的[J.加泰罗尼亚语,化学。物理335,69(2007)],其中辛二烯的1B(u)激发态由于扭曲不同的C-C单键而可产生两个不同的分子构象体。 (c)2008年美国物理研究所。

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