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首页> 外文期刊>Journal of Applied Physics >High pressure x-ray diffraction and extended x-ray absorption fine structure studies on ternary alloy Zn_(1-x)Be_(x)Se
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High pressure x-ray diffraction and extended x-ray absorption fine structure studies on ternary alloy Zn_(1-x)Be_(x)Se

机译:三元合金Zn_(1-x)Be_(x)Se的高压x射线衍射和扩展x射线吸收精细结构研究

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摘要

The ternary semiconductor alloy Zn_(1-x)Be_(x)Se has been studied under high pressure by x-ray diffraction and extended x-ray absorption fine structure (EXAFS) at the Zn and Se K-edge in order to determine the bulk and bond-specific elastic properties. Our measurements on samples with x = 0.06-0.55 show pressure induced phase transformation from zinc blende to NaCl. The phase transformation pressure increases linearly with x. Murnaghan equation of state fitting to the data yields the unit cell volume at ambient pressure and bulk modulus, both of which follow the Vegard's law. Nearest neighbor bond distances derived from EXAFS do not show sharp phase transition except for x= 0.06. Bond modulus derived for the Zn-Se bonds shows them to be apparently stiffer than the bulk alloy, which is nontrivial. This tendency increases with increasing x and a strong positive bowing from the Vegard's law is observed. We attribute the observed anomalies to the contrastingly different properties of the two components ZnSe and BeSe.
机译:通过高压X射线衍射和扩展的X射线吸收精细结构(EXAFS)在Zn和Se K边缘对三元半导体合金Zn_(1-x)Be_(x)Se进行了研究,以确定体积和结合特定的弹性。我们在x = 0.06-0.55的样品上进行的测量表明,压力诱导的相从锌共混物转变为NaCl。相变压力随x线性增加。拟合数据的Murnaghan状态方程可得出在环境压力和体积模量下的晶胞体积,这两者均遵循维加德定律。除了x = 0.06以外,从EXAFS导出的最近邻居键距都没有显示出明显的相变。从Zn-Se键获得的键模量显示它们明显比不重要的整体合金更坚硬。该趋势随着x的增加而增加,并且观察到了来自Vegard定律的强正弯曲。我们将观察到的异常归因于两种成分ZnSe和BeSe的不同特性。

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  • 来源
    《Journal of Applied Physics》 |2010年第8期|p.083533.1-083533.7|共7页
  • 作者单位

    Institut de Mineralogie et de Physique des Milieux Condenses, CNRS UMR 7590, Universite Pierre et Marie Curie-Paris 6, Campus Boucicaut, 140 rue de Lourmel, 75015 Paris, France;

    rnInstitut de Mineralogie et de Physique des Milieux Condenses, CNRS UMR 7590, Universite Pierre et Marie Curie-Paris 6, Campus Boucicaut, 140 rue de Lourmel, 75015 Paris, France;

    rnInstitut de Mineralogie et de Physique des Milieux Condenses, CNRS UMR 7590, Universite Pierre et Marie Curie-Paris 6, Campus Boucicaut, 140 rue de Lourmel, 75015 Paris, France;

    rnSynchrotron SOLEIL, L'Orme des Merisiers, Saint-Aubin, BP 48, 91192 Gif-sur-Yvette Cedex, France;

    rnSynchrotron SOLEIL, L'Orme des Merisiers, Saint-Aubin, BP 48, 91192 Gif-sur-Yvette Cedex, France;

    rnRaja Ramanna Centre for Advanced Technology, Indore 452013, India;

    rnRaja Ramanna Centre for Advanced Technology, Indore 452013, India;

    rnInstitut de Mineralogie et de Physique des Milieux Condenses, CNRS UMR 7590, Universite Pierre et Marie Curie-Paris 6, Campus Boucicaut, 140 rue de Lourmel, 75015 Paris, France;

    rnCPM-IJB, Universite Paul Verlaine, 57078 Metz, France;

    rnInstytut Fizyki, Uniwersytet Mikolaja Kopernika, Grudziadzka 5, 87-100 Torun, Poland;

    rnInstytut Fizyki, PAN, Al. Lotnikow 32/46, 02-668 Warszawa, Poland;

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