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首页> 外文期刊>The journal of physical chemistry, A. Molecules, spectroscopy, kinetics, environment, & general theory >Transient Phenomena in the Pulse Radiolysis of Oxoisoaporphine Derivatives in Acetonitrile
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Transient Phenomena in the Pulse Radiolysis of Oxoisoaporphine Derivatives in Acetonitrile

机译:乙腈中氧代异阿芬衍生物的脉冲辐解中的瞬态现象

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The absorption-spectral and kinetic behavior of radical ions and triplet states of two oxoisoaporphine derivatives, 2,3-dihydrooxoisoaporphine (2,3-DHOA) and 5-methoxy-2,3-dihydrooxoisoaporphine (5-MeO-2,3-DHOA), have been studied by UV-vis spectrophotometric pulse radiolysis in a neat acetonitrile saturated with argon and oxygen at room temperature. The radical anions of 2,3-DHOA and 5-MeO-2,3-DHOA are characterized by intense absorption maxima located at lambda(max) = 605 and 590 nm, with molar absorption coefficients epsilon(605) = 5600 M-1 cm(-1) and epsilon(590) = 4900 M-1 cm(-1), respectively. Both radical anions decay via first-order kinetics with the rate constants in the range (1.5-2.6) x 10(5) s(-1), predominantly through protonation by adventitious water forming neutral-hydrogenated radicals. Oxygen insensitive, the radical cations of 2,3-DHOA are characterized by a strong nondescript absorption band with no distinct lambda(max) in the range 350-450 nm. On the other hand, the radical cations of 5-MeO-2,3-DHOA are characterized by the distinctive absorption band with lambda(max) = 420 nm. The experimental spectra of the neutral-hydrogenated radicals and the triplet excited states derived from 2,3-DHOA and 5-MeO-2,3-DHOA are in accordance with the spectra observed previously during laser flash photolysis (De la Fuente, J. R.; et al. J. Phys. Chem. 2005, 109, 5897). Most of the transient spectra generated radiolytically are adequately reproduced by quantum mechanical semiempirical PM3 and ZINDO/S methods.
机译:两种氧代异阿波芬衍生物(2,3-dihydrooxoisoisoaporphine(2,3-DHOA)和5-甲氧基-2,3-dihydrooxoisoaporphine(5-MeO-2,3-DHOA)的自由基离子和三重态的吸收光谱和动力学行为),已通过在室温下用氩气和氧气饱和的纯乙腈中的紫外可见分光光度法脉冲辐解研究。 2,3-DHOA和5-MeO-2,3-DHOA的自由基阴离子的最大吸收峰位于lambda(max)= 605和590 nm,摩尔吸收系数epsilon(605)= 5600 M-1 cm(-1)和epsilon(590)分别为4900 M-1 cm(-1)。两个自由基阴离子都通过一级动力学以速率常数在(1.5-2.6)x 10(5)s(-1)范围内衰减,主要是通过不定水质子化形成中性氢化自由基而发生的。 2,3-DHOA对氧不敏感,其自由基阳离子具有很强的非描述性吸收带,在350-450 nm范围内没有明显的λ(max)。另一方面,5-MeO-2,3-DHOA的自由基阳离子具有独特的吸收带,λ(max)= 420 nm。由2,3-DHOA和5-MeO-2,3-DHOA衍生的中性氢自由基和三重激发态的实验光谱与先前在激光闪光光解过程中观察到的光谱一致(De la Fuente,JR;等人,J.Phys.Chem.2005,109,5897)。通过量子力学半经验PM3和ZINDO / S方法可以充分再现辐射分解产生的大多数瞬态光谱。

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