Elsevier

Physics Letters A

Volume 411, 30 September 2021, 127528
Physics Letters A

Lattice mismatch, mechanical properties and lattice-compensation effect in Si1-xGex alloys by using first-principles calculations combined with virtual crystal approximation

https://doi.org/10.1016/j.physleta.2021.127528Get rights and content

Highlights

  • Calculation by first-principles calculations combined with virtual crystal approximation.

  • Lattice parameters of Si1-xGex alloy with any concentration ratio.

  • Mechanical properties including elastic constants and moduli of Si1-xGex alloys.

  • Lattice-compensation effect in Si1-x-yGexBy ternary alloys.

Abstract

Si and Ge are two key semiconductor elements to construct CMOS-based devices and IC transistors, while the lattice mismatch of these two elements may decrease the quality and stability of heterojunction bipolar transistors based on Si1-xGex alloy. In this work, by using the first-principles calculations and the virtual crystal approximation (VCA) in material structures, we studied the lattice mismatch and the fundamental mechanical parameters in Si1-xGex alloys. The numerical results are consistent with those reported in some previous works. Moreover, the lattice-compensation effect induced by B-doping in Si1-xGex alloy is also studied, confirming further that the VCA is an efficient way to study the multi-component alloy systems doped by other kinds of atoms. Our work puts forward a feasible theoretical method to study the lattice constants, the lattice mismatch, the mechanical properties and the lattice-compensation effects in multi-component alloy systems.

Introduction

To design high-quality heterojunction bipolar transistors and COMS-based devices, one efficient way is to enhance the carrier mobility in the strain-induced layer of integrated circuit (IC) transistors [1], [2]. Usually, two typical semiconducting elements, Ge and Si, are adopted to construct the Si1-xGex alloy in these devices, where x denotes the mole ratio of Ge [3], [4], [5], [6], [7]. Owing to the advantage that these two elements are soluble with each other at any proportion, Si1-xGex alloys form a series of substitutional solid solutions distributed continuously with changing the parameter x. Thus, these alloy candidates have long been regarded as the most important raw materials to construct semiconducting devices. For example, we usually apply the alloy Si1-xGex to design the critical component, i.e., the strain-inducing layer in bipolar transistors, because their carrier mobility determines the signal sensitivities and accuracies of the transistors.

Although Si and Ge are face-centered cubic crystals, they host different lattice constants, which induce the lattice mismatch in the related semiconducting devices. On one hand, lattice mismatch serves as one important way to produce the strain-inducing layers between the epitaxial film and the substrates in COMS-based devices. For example, artificially induced lattice mismatch can be used to increase the carrier mobility in the channels of IC transistors, which is helpful to enhance the device sensitivity. On the other, the lattice mismatch between semiconductor layers may severely limit device application. As the lattice mismatch is beyond its appropriate value, the mismatch dislocation occurs usually in alloy materials, decreasing the device stability of IC transistors. It is noted that the lattice constant of single Ge crystal (aGe = 0.5658 nm) is larger than that of single Si crystal (aSi = 0.5431 nm) about 4.2%, indicating that the mismatch dislocation occurs easily in Si1-xGex alloy, as illustrated in Fig. 1. Thus, controlling the right lattice mismatch in the Si1-xGex alloys is of great importance for obtaining high-quality semiconducting materials towards high-efficient IC transistors. Furthermore, once the relationships between the lattice constants of Si1-xGex alloys and the concentration of Ge is understood, the lattice mismatch induced strain can be determined quantitatively in the epitaxial films [8], helping the experimentalists to perform the device optimizations of IC transistors [9].

In this work, by using first-principles calculations in combination with the virtual crystal approximation (VCA) method, we study the influence of the concentration of Ge on the lattice mismatch in the Si1-xGex alloys and explore their fundamental mechanical properties. Our theoretical results show that the lattice constants of the Si1-xGex alloy obtained by our theoretical calculations are well consistent with the previous results from Vegard's law [10] and the experimental results from Dismukes et al. [11], [12]. Moreover, some mechanical parameters including the elastic stiffness constants, bulk, shear and Young's modulus and Poisson's ratio of the Si1-xGex alloy are also obtained and discussed. Finally, by using the same theoretical methods, the B-doped Si1-xGex alloys, i.e., the SiGeB ternary alloys are studied. The B-doping induced lattice-compensation effect is also discussed. These numerical results show that our first-principles calculations combined with the VCA can be applied as an efficient way to study the lattice mismatch, the mechanical properties and the lattice-compensation effects of multi-component alloy systems.

The reminder of this paper is organized as follows. In Section 2, the model of Si1-xGex alloy within VCA and the related theoretical methods are introduced in details. In Section 3, the numerical results of the lattice mismatch and some mechanical parameters are obtained and then, the lattice-compensation effect induced by B-doping in Si1-xGex alloy is discussed in details. Finally, the main results are summarized in the last section.

Section snippets

The alloy model and calculation methods

For multi-component alloy systems, we usually construct the realistic crystal structure by using atom substitution in a united cell. Nevertheless, this approach has an obvious disadvantage that it is difficult to ensure the uniformity of the spatial distribution of substituted atoms. Especially, in order to illustrate a rare element doping in the alloy, the supercell of the alloy example should be extended to a much large one, which increases largely the difficulty to perform the

The lattice constants of Si1-xGex alloys obtained by the DFT combined with the VCA

To the present, there are several different methods to calculate the lattice contents of Si1-xGex alloys by changing the component ratio of Ge. One of them is to predict approximately the lattice contents of alloy systems by an experiential Vegard's law [10], [31], which describes the lattice content a of the Si1-xGex alloys in the following expression.a=(1x)aSi+xaGe=5.431(1x)+5.658x(Å). Note that the Vegard's law is a rather simple way to estimate the lattice constants of an alloy, because

Conclusions

In summary, by using the first-principles calculations within the framework of VCA, the lattice constants, the lattice mismatch and several mechanical properties of the Si1-xGex alloys were studied systemically, the numerical results are consistent with those reported in some previous theoretical and experimental works. Moreover, we found that the VCA is an efficient way to study the multi-component alloy systems doped by other kinds of atoms. Besides, we extended the theoretical methods and

CRediT authorship contribution statement

Yingjie Cai: Conceptualization, Data curation, Formal analysis, Investigation, Methodology, Software, Validation, Visualization, Writing – original draft, Writing – review & editing. Chaoying Xie: Conceptualization, Methodology, Project administration, Resources, Software, Supervision, Writing – review & editing.

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

The authors would like to acknowledge the Shanghai Jiao Tong University and the School of Material Science and Engineering of Shanghai Jiao Tong University for the technical supports.

References (42)

  • Y. Arai et al.

    J. Cryst. Growth

    (2021)
  • B. Winkler et al.

    Chem. Phys. Lett.

    (2002)
  • E. Kasper et al.

    J. Cryst. Growth

    (1995)
  • C. Wu et al.

    Chin. J. Phys.

    (2020)
  • X.-Z. Lu et al.

    Nat. Mater.

    (2016)
  • J. Falta et al.

    Appl. Phys. Lett.

    (1997)
  • M. Mamor et al.

    J. Appl. Phys.

    (2019)
  • M. Montanari et al.

    Appl. Phys. Lett.

    (2021)
  • T. Ozawa et al.

    J. Appl. Phys.

    (2021)
  • A. Anam et al.

    IEEE Sens. J.

    (2020)
  • Y.S. Li et al.

    ACS Nano

    (2015)
  • H. Fang et al.

    Proc. Natl. Acad. Sci. USA

    (2013)
  • L. Vegard

    Z. Phys.

    (1921)
  • J.P. Dismukes et al.

    J. Phys. Chem.

    (1964)
  • J. Dismukes et al.

    J. Appl. Phys.

    (1964)
  • L. Bellaiche et al.

    Phys. Rev. B

    (2000)
  • N.J. Ramer et al.

    Phys. Rev. B

    (2000)
  • G. Geneste et al.

    Phys. Rev. B

    (2008)
  • B. Hammer et al.

    Phys. Rev. B

    (1999)
  • P. Geerlings et al.

    Chem. Rev.

    (2003)
  • E. Kasper et al.

    Properties of Silicon Germanium and SiGe: Carbon

    (2000)
  • Cited by (6)

    View full text