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Stranski-Krastanov mechanism of growth and the effect of misfit sign on quantum dots nucleation

机译:Stranski-Krastanov的生长机理以及失配符号对量子点成核的影响

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The thermodynamics of the Stranski Krastanov mode of epitaxial growth and the effect of the sign of the lattice misfit are discussed. The Stranski Krastanov mode of growth represents a sequence of layer-by-layer or Frank-van der Merwe growth followed by the formation of three-dimensional (3D) islands or Volmer Weber growth. The occurrence of both growth modes mentioned above is in compliance with the wettability criterion of Bauer. The positive wetting function required for the occurrence of the Volmer Weber growth is originated by the vertical displacements of the atoms close to the edges of the two-dimensional (2D) islands as a result of the relaxation of the lattice misfit. The monolayer high islands become unstable against bilayer islands, bilayer islands in turn become unstable against trilayer islands, etc. beyond some critical islands sizes. Monolayer islands appear as necessary precursors of three-dimensional (3D) islands. The critical island size for mono-bilayer transformation increases steeply with decreasing lattice misfit and diverges at a critical value of the misfit. This value divides the regions of Frank-van der Merwe and Stranski Krastanov modes in a phase diagram of coordinates wetting-misfit. The transformation of monolayer to multilayer islands takes place either by consecutive nucleation and growth of 2D islands (layer-by-layer transformation), or by nucleation and lateral (2D) growth of multilayer islands (multilayer 2D transformation). The former occurs in the case of "stiff" overlayer materials and mostly in compressed overlayers. The latter takes place in the case of "soft" materials like Pb and In, mostly in tensile overlayers. Tensile films show non-nucleation transformation compared with the nucleation-like behavior of compressed films. (C) 2017 Elsevier B.V. All rights reserved.
机译:讨论了Stranski Krastanov外延生长模式的热力学以及晶格失配符号的影响。 Stranski Krastanov的增长模式表示一系列的逐层增长或Frank-van der Merwe增长,然后形成三维(3D)岛或Volmer Weber增长。上述两种生长方式的出现均符合鲍尔(Bauer)的润湿性标准。发生Volmer Weber增长所需的正润湿函数是由于晶格失配弛豫的结果,靠近二维(2D)岛的边缘的原子的垂直位移而产生的。单层高岛对双层岛变得不稳定,双层岛又对三层岛变得不稳定,等等,超过了一些临界岛的大小。单层岛似乎是三维(3D)岛的必要前体。单双层转化的临界岛尺寸随着晶格失配的减少而急剧增加,并以失配的临界值发散。此值在坐标润湿不匹配的相图中划分了Frank-van der Merwe模式和Stranski Krastanov模式的区域。单层到多层岛的转变可以通过2D岛的连续成核和生长(逐层转换)进行,也可以通过多层岛的成核和横向(2D)生长(多层2D转变)进行。前者发生在“硬”覆盖层材料的情况下,并且多数发生在压缩覆盖层中。后者发生在“软”材料(如Pb和In)的情况下,大多数情况下在拉伸覆盖层中。与压缩膜的成核样行为相比,拉伸膜显示出非成核转变。 (C)2017 Elsevier B.V.保留所有权利。

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  • 来源
    《Surface Science》 |2017年第10期|172-184|共13页
  • 作者

    Prieto J. E.; Markov I.;

  • 作者单位

    Univ Autonoma Madrid, IFIMAC, Dept Fis Mat Condensada, Ctr Microanal Mat, E-28049 Madrid, Spain|Univ Autonoma Madrid, Inst Univ Nicolas Cabrera, E-28049 Madrid, Spain;

    Bulgarian Acad Sci, Inst Phys Chem, BU-1113 Sofia, Bulgaria;

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