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Phase selection and transition in Hf-rich hafnia-titania nanolaminates

机译:富H的二氧化钛纳米层压板的相选择和过渡

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Hf-rich hafnia-titania nanolaminate films with five HfO_2-TiO_2 bilayer architectures (0.64 to 0.94 Hf atom fraction) were sputter deposited on unheated fused silica substrates, annealed post-deposition from 573 to 1273 K, and analyzed by x-ray diffraction to study phase selection and transition. Isochronal annealing for 1 h intervals from 573 to 1173 K produces weak crystallization into monoclinic (m) HfO_2 doped with Ti, i.e., m-Hf_(1-x)Ti_xO_2. The amount of Ti incorporated into m-HfO_2 depends upon both architecture and overall stoichiometry, but in all but the coarsest architecture, exceeds the bulk solubility limit of x = 0.05. Initial annealing at 1273 K produces significant crystallization into a biphasic structure, m-Hf_91-x)Ti_xO_2 and orthorhombic (o) HfTiO_4. From bulk phase equilibrium considerations, o-HfTiO_4 is expected to crystallize under conditions of interfacial bilayer mixing. However, upon further annealing at 1273 K, o-HfTiO_4 proves to be unstable. o-HfTiO_4 demixing inevitably occurs independent of architecture and stoichiometry, resulting in final crystallization products after 96 h at 1273 K that are m-Hf_(1-x)Ti_xO_2 with x ≈ 0.05 and TiO_2 doped with Hf. We suggest that o-HfTiO_4 instability arises from a driving force to form domains similar to those found in the low temperature in/commensurate structures of ZrTiO_4. A detailed crystallographic group-subgroup analysis of the o (Pbcn) → m (P2_1/c) transition shows that these domains can be represented by an orientation twin in the latter structure and their creation can be achieved by a single step second-order phase transition.
机译:将具有五种HfO_2-TiO_2双层结构(0.64至0.94 Hf原子分数)的富Hf氧化钛-氧化钛纳米层压膜溅射沉积在未加热的熔融石英基板上,退火后沉积573至1273 K,并通过X射线衍射分析到研究阶段选择和过渡。从573到1173 K等时退火1 h间隔会产生微弱的结晶,变成掺有Ti的单斜晶(m)HfO_2,即m-Hf_(1-x)Ti_xO_2。 Ti掺入m-HfO_2的量取决于结构和总体化学计量,但除最粗糙的结构外,其余所有量均超过x = 0.05的整体溶解度极限。在1273 K处进行初始退火会产生明显的结晶,形成双相结构,即m-Hf_91-x)Ti_xO_2和正交晶(o)HfTiO_4。从体相平衡的考虑,预期o-HfTiO_4在界面双层混合的条件下结晶。然而,在1273 K下进一步退火后,o-HfTiO_4被证明是不稳定的。不可避免地发生o-HfTiO_4分解,而与结构和化学计量无关,导致在1273 K下96 h后最终结晶产物为x≈0.05的m-Hf_(1-x)Ti_xO_2和TiO_2掺杂的Hf。我们建议,o-HfTiO_4的不稳定性是由形成类似于ZrTiO_4的低温/相称结构中发现的域的驱动力引起的。 o(Pbcn)→m(P2_1 / c)跃迁的详细晶体学-亚组分析表明,这些结构域可以由后一种结构中的取向孪晶表示,并且它们的生成可以通过一步法二阶相完成过渡。

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  • 来源
    《Journal of Applied Physics 》 |2011年第12期| p.318-325| 共8页
  • 作者单位

    Department of Chemistry and Biochemistry University of Wisconsin-Milwaukee, P.O. Box 413, Milwaukee, Wisconsin 53201, USA;

    Department of Chemistry and Biochemistry University of Wisconsin-Milwaukee, P.O. Box 413, Milwaukee, Wisconsin 53201, USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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