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Piezo-spectroscopic behavior of the emission bands of α-alumina in the 13900–14250 cm− 1 spectral range

机译:13900-14250 cm-1 光谱范围内α-氧化铝发射带的压电光谱行为

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摘要

The emission spectrum of α-alumina in the spectral range between 13900 and 14250 cm−1 is characterized by several bands which are much weaker than the two intense and sharp R1 and R2 bands appearing at 14400 and 14430 cm−1, respectively; these latter are known as Ruby lines and they are the emission bands used in the Ruby laser. Furthermore these bands shift in frequency with stress (Piezo-Spectroscopic effect). In this paper, for the first time, the stress-dependent peak frequency of the weaker bands in the 13900–14250 cm−1 range is calibrated, and the results are presented as Piezo-Spectroscopic coefficients. The calibration is performed by reporting the frequency shift of each investigated band as function of varying stresses. The stresses, residual in nature, are obtained by fabricating composite materials where α-alumina is mixed in various amounts with (i) Ceria-Stabilized Tetragonal Zirconia Polycrystals (Ce-TZP) and (ii) silicon carbide, SiC. The composite materials are prepared at high temperature (1500°–1800°C); due to the difference in thermal expansion, upon cooling to room temperature α-alumina develops compressive and tensile stresses, when mixed with Ce-TZP and SiC, respectively. The stress values necessary for the calibration are obtained from the frequency shift of the R2 band, using its well-established Piezo-Spectroscopic coefficient (7.6 cm−1/GPa). Then the newly obtained Piezo-Spectroscopic coefficients of the bands in the 13900–14250 cm−1 range are tested to retrieve the stresses in two sets of composites; finally the stress values are compared with those obtained in the same samples from the frequency shift of the R2 band. The comparison shows a very good agreement, thus providing evidence that the bands in the 13900–14250 cm−1 range can be used to monitor stresses in α-alumina-based materials.
机译:α-氧化铝在13900和14250 cm-1 光谱范围内的发射光谱的特征是几个波段远弱于出现在14400和14430 cm-1 分别;后者被称为红宝石线,它们是红宝石激光器中使用的发射带。此外,这些频带随着应力的变化而发生频率变化(压电分光效应)。本文首次校准了13900–14250 cm-1 范围内较弱带的应力相关峰值频率,并将结果表示为压电光谱系数。通过报告每个调查频段的频移作为变化应力的函数来执行校准。本质上残余的应力是通过制造复合材料获得的,其中将α-氧化铝与(i)二氧化铈稳定的四方氧化锆多晶体(Ce-TZP)和(ii)碳化硅SiC混合在一起。复合材料在高温(1500°–1800°C)下制备;由于热膨胀的差异,当冷却至室温时,α-氧化铝分别与Ce-TZP和SiC混合时会产生压缩应力和拉伸应力。校准所需的应力值是使用R2波段的频偏系数(7.6 cm-1 / GPa)从R2波段的频移获得的。然后测试新获得的13900–14250 cm-1 范围内的带的压电光谱系数,以恢复两组复合材料中的应力。最后,将应力值与从R2频带的频移获得的相同样本中的应力值进行比较。比较显示出很好的一致性,因此提供了证据表明13900–14250 cm-1 范围内的谱带可用于监视基于α-氧化铝的材料中的应力。

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  • 来源
    《Journal of Materials Science》 |2005年第7期|1593-1597|共5页
  • 作者单位

    Department of General and Inorganic Chemistry Baku State University;

    CENMAT Center of Excellence for Nanomaterials and Nanostructured Surfaces University of Trieste;

    CENMAT Center of Excellence for Nanomaterials and Nanostructured Surfaces University of Trieste;

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