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Effect of low NiO doping on anomalous light scattering in zinc aluminosilicate glass-ceramics

机译:低NIO掺杂对铝硅酸盐玻璃陶瓷异常光散射的影响

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Abstract The effect of low NiO doping (0–0.15mol%) on the extinction coefficient of zinc aluminosilicate glass-ceramics prepared by five different two-stage heat treatments was studied experimentally. Extinction coefficient vs wavelength presented as a log-log plot was separated into scattering and absorption coefficients. The NiO addition drastically changes not only values of the scattering coefficient at a given wavelength of visible light (effect 1), but also the type of wavelength dependence of this coefficient (effect 2). These effects do not correlate with variation of sizes and volume fractions of nanocrystals determined by Rietveld refinement of X-ray diffraction data. They cannot be described in the model of independent Rayleigh scatterers. These effects are characteristic features of anomalous light scattering by inhomogeneous glasses and can be explained by interference of light scattered by different nanocrystals. To calculate interference effects, the detailed information on mutual arrangement of nanocrystals is required, which unlikely can be determined experimentally for multiphase polydisperse system of nanocrystals. Instead, simplified models for systems of nanocrystals in glass-ceramics can be considered. And finally, we cannot explain the mechanism of the effect of small NiO additions on light scattering and hence, on structure of glass-ceramics. Highlights ? Zinc aluminosilicate glass-ceramics doped with 0–0.15mol% NiO were studied. ? Extinction coefficient was separated into scattering and absorption coefficients. ? Extremely low NiO addition (0.01–0.05mol%) drastically decreases light scattering. ? Observed scattering is much less than that calculated for independent scatterers. ? Anomalies in light scattering are connected with interference effects. ]]>
机译:<![cdata [ 抽象 低NIO掺杂的效果(0-0.15 Mol% )通过实验研究了五种不同的两级热处理制备的锌硅酸盐玻璃陶瓷的消光系数。作为对数图呈现的消光系数Vs波长被分离成散射和吸收系数。 NIO添加的不仅在可见光(效果1)的给定波长处的散射系数的值大大变化,而且还具有该系数的波长依赖性的类型(效果2)。这些效果与通过RIETVELD细化X射线衍射数据确定的纳米晶体的尺寸和体积分数的变化不相关。他们不能在独立的瑞利散射体模型中描述。这些效果是非均匀玻璃的异常光散射的特征特征,并且可以通过不同纳米晶体散射的光的干涉来解释。为了计算干扰效果,需要有关纳米晶体相互布置的详细信息,这不太可能在实验上实验确定纳米晶体的多相多分散系统。相反,可以考虑玻璃陶瓷中纳米晶体系统的简化模型。最后,我们无法解释小型NIO添加对光散射的影响的机制,从而实现玻璃陶瓷的结构。 亮点 镀锌玻璃玻璃陶瓷掺杂0-0.15 MOL%NIO。 消光系数分成散射和吸收系数。 e Xtremely Low Nio添加(0.01-0.05 Mol%)大大降低了光散射。 观察到的散射远小于独立散射仪计算的散射。 光散射中的异常与干扰效果有关。 ]]>

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