γ辐照正构烷烃单晶中烷基自由基的分布、结构和性质显示了固体中辐射能量的沉积

Tomas Gillbro, Anders Lund
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引用次数: 35

摘要

本文综述了γ辐照正构烷烃单晶的esr研究结果。它还包含了一些新的实验结果,这些结果有助于更全面地了解辐射能量在固体烷烃中的沉积。用固体正构烷烃进行的实验迄今为止提供了结构数据,使人们能够清楚地了解烷基自由基的性质甚至构象。存在两种类型的自由基,一种是未配对电子位于末端甲基附近,另一种是未配对电子位于链的内部。第一类分子的构象与未受损分子的构象不同。微波饱和数据表明,这些自由基的弛豫特性存在差异,这可以用迁移率的差异来理解。相对产率测量给出了同分异构体烷基的分布,结果不同于在液体中使用产物分析得到的结果。对于质子化的正构烷烃,正烷基缺乏,2-烷基浓度高于预期。对于氘化正构烷烃,电磁共振谱主要是未配对电子位于碳链内部的自由基的电磁共振谱。这种同位素效应再次与在液态正构烷烃中的观察结果相反。在77 K辐照的质子化烷烃和4.2 K辐照的氘化烷烃中观察到的宽谱线不认为是由强自旋-自旋相互作用引起的。相反,它们被认为是由扭曲的晶体和与晶体损伤区域有关的自由基结构引起的。自由基对的存在具有不同的稳定性、产率和结构。我们估计,在氘化烷烃中,高达40%的自由基在4.2 K时形成成对或簇状,这表明自由基对的形成是固体正构烷烃中一个重要的辐射分解过程。从氘化分子到质子化分子的能量转移也得到了实验验证。这种能量转移与温度有关,在77 K时有效,但在4.2和273 K时效率较低。氘化烷烃在4k时形成的自由基对数量与77k时的远程能量转移之间也存在关系。这可以很容易地用类似于芳香晶体中的激子转移机制来解释。它也可以定性地描述为氢提取过程。然而,在这种情况下,氘原子的性质尚不清楚。
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Deposition of radiation energy in solids as visualized by the distribution, structure and properties of alkyl radicals in γ-irradiated n-alkane single crystals

This paper summarizes results obtained earlier from E.S.R. studies of γ-irradiated n-alkane single crystals. It also contains some new experimental results that serve to give a more complete picture of the deposition of radiation energy in solid alkanes. The experiments performed with solid n-alkanes have thus far provided structural data that permit the nature and even the conformation of alkyl radicals to be clearly understood. Two types of radical exist, namely, one where the unpaired electron is located next to the end methyl group and one with the unpaired electron in the interior of the chain. The first type has a conformation which differs from that of the undamaged molecule. Microwave saturation data show that there is a difference in relaxation properties of these radicals which can be understood in terms of a difference in mobility. Relative yield measurements give the distribution of isomeric alkyl, the result differing from that obtained using product analysis in liquids. For protiated n-alkanes n-alkyl is lacking and the 2-alkyl concentration is higher than expected. For deuterated n-alkanes the E.S.R. spectrum is mainly that of radicals with the unpaired electron located in the interior of the carbon chain. This isotope effect is again contrary to observations in liquid n-alkanes.

The broad lines observed in protiated alkanes irradiated at 77 K and deuterated alkanes irradiated at 4.2 K are not believed to arise from strong spin-spin interactions. They are thought instead to arise from distorted crystal and radical structures relating to the damage regions of the crystals.

Radical pairs exist with different stability, yield and structure. Our estimate, in deuterated alkanes, that as much as 40% of the radicals are formed in pairs or clusters at 4.2 K shows that radical pair formation is an important radiolytic process in solid n-alkanes. Energy transfer from deuterated to protiated molecules has also been experimentally verified. This energy transfer is temperature dependent and occurs efficiently at 77 K, but less efficiently at 4.2 and 273 K. A relationship also exists for deuterated alkanes between the amount of radical pairs formed at 4 K and the long-range energy transfer at 77 K. This can be readily accounted for by an exciton transfer mechanism analogous to that in aromatic crystals. It might also be qualitatively described by a hydrogen abstraction process. In this case, however, the properties of the deuterium atoms are not understood.

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