CEA, DEN, SRMA, 91191 Gif-sur-Yvette Cedex, France.
J Phys Condens Matter. 2010 Aug 11;22(31):315402. doi: 10.1088/0953-8984/22/31/315402. Epub 2010 Jul 16.
We have studied the colour centre production in yttria-stabilized zirconia (ZrO(2):Y(3 +)) by heavy ion irradiation in the GeV range using on-line UV-visible optical absorption spectroscopy. Experiments were performed with 11.4 MeV amu(-1) (127)Xe, (197)Au, (208)Pb and (238)U ion irradiations at 8 K or room temperature (RT). A broad and asymmetrical absorption band peaked at a wavelength about 500 nm is recorded regardless of the irradiation parameters, in agreement with previous RT irradiations with heavy ions in the 100 MeV range. This band is de-convoluted into two broad Gaussian-shaped bands centred at photon energies about 2.4 and 3.1 eV that are respectively associated with the F(+)-type centres (involving a singly ionized oxygen vacancy, VO· and T centres (i.e. Zr(3+) in a trigonal symmetry) observed by electron paramagnetic resonance (EPR) spectroscopy. In the case of 8 K Au ion irradiation at low fluences, six bands are used at about 1.9, 2.3, 2.7, 3.1 and 4.0 eV. The three bands near 2.0-2.5 eV can be assigned to oxygen divacancies (i.e. F(2)(+) centres). No significant effect of the irradiation temperature is found on the widths of all absorption bands for the same ion and fluence. This is attributed to the inhomogeneous broadening arising from the static disorder due to the native charge-compensating oxygen vacancies. However, the colour centre production yield is strongly enhanced at 8 K with respect to RT. When heating irradiated samples from 8 K to RT, the extra colour centres produced at low temperature do not recover completely to the level of RT irradiation. The latter results are accounted for by an electronically driven defect recovery process.
我们使用在线紫外-可见吸收光谱研究了 GeV 范围内重离子辐照稳定氧化锆(ZrO2:Y3+)中的色心生成。实验是在 8 K 或室温(RT)下,用 11.4 MeV amu-1(127)Xe、(197)Au、(208)Pb 和(238)U 离子辐照进行的。无论辐照参数如何,都会记录到一个宽且不对称的吸收带,其峰值位于约 500nm 的波长处,这与之前在 100 MeV 范围内用重离子进行的 RT 辐照结果一致。该带通过解卷积成两个宽的高斯形带,中心位于约 2.4 和 3.1 eV 的光子能量处,分别与电子顺磁共振(EPR)光谱观察到的 F+-型中心(涉及单电离氧空位 VO·和 T 中心(即三配位的 Zr3+)有关。在低剂量 8 K Au 离子辐照的情况下,使用了约 1.9、2.3、2.7、3.1 和 4.0 eV 的六个带。靠近 2.0-2.5 eV 的三个带可以分配给氧双空位(即 F2+中心)。对于相同的离子和剂量,辐照温度对所有吸收带的宽度没有明显影响。这归因于由于固有电荷补偿氧空位引起的静态无序引起的非均匀展宽。然而,与 RT 相比,色心生成产率在 8 K 时得到了显著增强。当将辐照样品从 8 K 加热到 RT 时,低温下产生的额外色心不会完全恢复到 RT 辐照的水平。后一种结果归因于电子驱动的缺陷恢复过程。