Journal of Semiconductors, Volume. 45, Issue 10, 102101(2024)

Impact of strain relaxation on the growth rate of heteroepitaxial germanium tin binary alloy

Pedram Jahandar* and Maksym Myronov
Author Affiliations
  • Department of Physics, University of Warwick, Coventry, CV4 7AL, United Kingdom
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    Figures & Tables(6)
    (Colour online) Theoretical calculations of hc for Ge1–ySny films grown on Si substrate via a relaxed Ge-VS using the People Bean (P–B) model and the Matthew Blakeslee (M–B) model[13]. Experimental data collected from this work as well as previous research are included[14−16].
    (Colour online) (a) HR-XRD ω–2θ coupled scans for Ge1–ySny epilayers grown with different growth times on Si (001) via Ge-VS. Symmetric and asymmetric RSMs for Ge1–ySny grown with different growth times on Si (001) via Ge-VS of (b) 79 nm thick Ge0.884Sn0.116 grown for 8 min, (c) 95 nm thick Ge0.884Sn0.116 grown for 10 min, (d) 128 nm thick Ge0.882Sn0.118 grown for 15 min, and (e) 150 nm thick Ge0.878Sn0.122 grown for 20 min. The Sn concentration for each of these samples was measured from RSMs and using the modified Vegard’s law. The thicknesses of these epilayers are measured using either thickness fringes appeared in their HR-XRD ω–2θ coupled scans or X-TEM images, as shown in the example in Fig. 3(a).
    (Colour online) (a) X-TEM image of 150 nm thick Ge0.878Sn0.122 grown on Ge-VS. The high resolution lattice resolved X-TEM micrographs of Ge0.878Sn0.122/Ge-VS interface as well as surface of Ge0.878Sn0.122 epilayer are presented. (b) Relationship between thickness, Sn concentration and total growth rate of Ge1–ySny epilayers. (c) AFM scan of 95 nm thick Ge0.884Sn0.116. (d) AFM scan of 128 nm thick Ge0.882Sn0.118. (e) AFM scan of 150 nm thick Ge0.878Sn0.122. (f) Surface roughness (RMS) of Ge1–ySny epilayers with different thicknesses. Surface roughness increased with the increase in thickness (growth time), particularly after the critical thickness of ~95 nm.
    (Colour online) (a) Average growth rate (nm/min) at the given thickness (nm) of the Ge1–ySny and its corresponding growth time (min). As the thickness of the Ge1–ySny increases, the growth rate decreases. (b) Actual data points collected experimentally for average growth rate (nm/min).
    (Colour online) The effect of strain relaxation in Ge1–ySny epilayers on their growth rate. The growth rate at given strain relaxation state was estimated using the fitted line to the actual data points given in Fig. 4. In-plane and out-of-plane strain were calculated by Eqs. (1) and (2).
    • Table 1. Summary of effects of strain relaxation on the Sn concentration and growth rate of Ge1–ySny epilayers grown at 260 °C and 500 Torr on Si (001) via a relaxed Ge-VS.

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      Table 1. Summary of effects of strain relaxation on the Sn concentration and growth rate of Ge1–ySny epilayers grown at 260 °C and 500 Torr on Si (001) via a relaxed Ge-VS.

      Thickness (nm)In-plane strain (10–3)Out-of-plane strain (10–3)Average Sn content (at.%)Average growth rate (nm/min)
      29–15.412.111.69.7
      50–15.612.211.610.0
      79–15.812.411.69.9
      95–15.612.311.69.5
      128–11.18.711.88.5
      150–9.87.712.27.5
      –9.37.312.5
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    Pedram Jahandar, Maksym Myronov. Impact of strain relaxation on the growth rate of heteroepitaxial germanium tin binary alloy[J]. Journal of Semiconductors, 2024, 45(10): 102101

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    Paper Information

    Category: Research Articles

    Received: Mar. 4, 2024

    Accepted: --

    Published Online: Dec. 5, 2024

    The Author Email: Jahandar Pedram (PJahandar)

    DOI:10.1088/1674-4926/24030002

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