Luminescence de recombinaison consecutive a la photoionisation d'une solution organique vitreuse-nouvelle methode experimentale

D. Ceccaldi
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引用次数: 2

Abstract

In this paper, we describe a new experimental method which is used to determine the effect of temperature on the mechanisms related to the detrapping of electrons trapped in a glass. The studied samples are organic vitreous solutions of an aromatic molecule (TMPD) inside a non-polar glass (3-MP or MCH). The intensity of the isothermal luminescence (ITL) following the photoionization of the sample at 77K is increased when applying thermal jumps ΔT≲2K (the rise time is ⋍s).

A general kinetical theory is used to explain the shapes of the luminescence curves perturbed by thermal jumps. It is shown that the experimental observations can be explained in terms of a slow diffusion of the trapped electrons towards a tunneling detrapping zone. When applying a thermal jump ΔT, the intensity of luminescence is multiplied by X such as: X = exp ΔTTEkT+ Y1+Y.

This relationship is in good agreement with experience. The thermal detrapping activation energy E and the tunnelling effect ratio Y can be determined through this formula. The shapes of the kinetic curves at T = 77K and T = 77·50K are compared in the case of 3-MP glassy samples (near the glass transition, Tg = 77K). It is concluded that there is a slow diffusion of trapped electrons (as it was already shown); the diffusion activation energy (Ed = 0·65eV) is found to be very close to viscosity activation energy (E = 0·65eV) as given by Willard. This last result seems to support the hypothesis according to which the diffusion of trapped electrons is the consequence of the diffusion of the trapping cavities (at Tg).

有机玻璃溶液光离子化后的连续复合发光-一种新的实验方法
在本文中,我们描述了一种新的实验方法,用于确定温度对玻璃中被困电子脱陷机制的影响。所研究的样品是芳香分子(TMPD)在非极性玻璃(3-MP或MCH)中的有机玻璃溶液。当施加热跳变ΔT > 2K(上升时间⋍s)时,样品在77K光离后的等温发光(ITL)强度增加。用一般动力学理论解释了热跃迁扰动下的发光曲线的形状。结果表明,实验结果可以用捕获电子向隧穿脱陷区缓慢扩散来解释。当应用热跳ΔT时,发光强度乘以X,如:X = exp ΔTTEkT+ Y1+Y。这种关系很符合经验。通过该公式可以确定热脱陷活化能E和穿隧效应比Y。比较了3-MP玻璃样品(接近玻璃化转变,Tg = 77K)在T = 77K和T = 77·50K时的动力学曲线形状。结论是,被捕获的电子有一个缓慢的扩散(正如已经显示的那样);发现扩散活化能(Ed = 0·65eV)与Willard给出的粘度活化能(E = 0·65eV)非常接近。最后一个结果似乎支持了一个假设,根据这个假设,被捕获电子的扩散是被捕获空腔扩散的结果(在Tg)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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