Ce3+在第三族金属氧化物中的电子激发

B. Namozov, V. Vetrov, S. Muradov, R. I. Zakharchenya
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引用次数: 1

摘要

在稀土离子中,Ce3+具有最简单的电子构型- 4f1。它的4f-5d跃迁的能量约为6.3 eV,这是完全允许的。因此,在具有足够宽禁隙的晶体中引入Ce3+,可以分析晶格环境对激发态的影响。在本研究中,通过对各种第三族金属氧化物中Ce3+杂质激发态的光谱动力学研究,得到了以下结果:(a)在所研究的氧化物中Ce3+的发光光谱具有双重态结构。这是由于自旋轨道相互作用导致Ce3+基态的2F5/2和2F7/2项能量分裂所致。(b)在Al2O3中,Ce3+发光激发光谱的长波区存在4f-5d跃迁对应的宽5组分带。在激发谱的短波区,可以消除一个非结构化的带,该带假设由激子带和电荷转移带组成,以及一个突出的窄激子带。(c) YAP中4f-5d跃迁在激发谱上分为两组:4-5 eV区域的3组分和5-6 eV区域的2组分。(d) YaG 4f-5d的跃迁在激发谱中分别为2.9、3.9、4.6、5.6、6.6 eV。由于YAG中基谱吸收边的紧密性,6.6 eV波段只能在低温下观测到。(e)在100 K以下的温度下,并没有检测到所有晶体从激子到杂质的能量转移。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electron excitation of Ce3+ in third group metal oxides
Among rare-earth ions Ce3+ has the simplest electron configuration - 4f1. Its 4f-5d transitions have an energy of approximately 6.3 eV for a free ion and are quite allowed. Thus, the introduction of Ce3+ into the crystal with wide enough forbidden gap makes it possible to analyze the lattice environment influence on the excited state. During the present research the following results were obtained via spectral-kinetic investigations of the excited states of Ce3+ impurity in various third group metal oxides: (a) luminescence spectrum of Ce3+ has a doublet structure in all examined oxides. This happens due to the energy split of 2F5/2 and 2F7/2 terms of Ce3+ ground state by reason of spin-orbit interaction. (b) In Al2O3 a broad 5-component band corresponding to 4f-5d transitions is observed in the long- wave region of Ce3+ luminescence excitation spectrum. In the short-wave region of excitation spectrum, one can eliminate a non-structured band, which hypothetically consists of the exciton band and the charge transfer band, and as well as an outstanding narrow exciton-band. (c) In YAP bands of 4f-5d transitions are divided into two groups in excitation spectrum: 3-component in the region of 4-5 eV and 2-component in the region of 5-6 eV. (d) In YaG 4f-5d transitions appear as separate bands in excitation spectrum: 2.9, 3.9, 4.6, 5.6, 6.6 eV. Due to the closeness of the fundamental absorption edge in YAG, the band 6.6 eV is observable only at low temperatures. (e) At temperatures under 100 K the energy transfer form exciton to impurity is not detected for all the crystals.
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