Evolution of thermal, structural, and optical properties of SiGe superlattices upon thermal treatment

• Published in: Physica status solidi. A, Applications and materials science Applications and materials science, 2016-03, Vol.213 (3), p.533-540
• Main Authors: Chen, Peixuan, Etzelstorfer, Tanja, Hackl, Florian, Katcho, Nebil A., Chang, Hung-Tai, Nausner, Lukas, Lee, Sheng-Wei, Fromherz, Thomas, Stangl, Julian, Schmidt, Oliver G., Mingo, Natalio, Rastelli, Armando
• Format: Article
• Language: English
• Subjects: 3-omega method; alloys; Annealing; Evolution; Heat transfer; Heat treatment; photoluminescence; SiGe; Silicon germanides; Superlattices; Thermal conductivity; Transmission electron microscopy
• ISSN: 1862-6300; 1862-6319
• DOI: 10.1002/pssa.201532468

We investigate the evolution of the cross‐plane thermal conductivity κ of a SiGe superlattice (SL) as it is gradually converted into an alloy via post‐growth thermal treatment at temperatures varying from 650 to 1000 °C. X‐ray diffraction (XRD), transmission electron microscopy (TEM), secondary‐ion‐mass‐spectroscopy (SIMS), and photoluminescence (PL) spectroscopy measurements are used as complementary tools to gain insight into the structural properties of our SL and their evolution upon annealing. While the SL structure is preserved up to temperatures of ∼850 °C, full alloying is observed for higher temperatures. The thermal conductivity data, collected with differential 3ω method, show a monotonic increase of κ from ∼4.5 W/m K up to the values expected for a thin‐film alloy. To understand the results, we compute the phonon mean‐free‐path (MFP) spectra using the experimentally determined composition profiles as input. The calculated thermal conductivity values are in good agreement with the experimental data and show that the increase of thermal conductivity is due to a gradual increase of MFP of low‐to‐mid‐frequency phonons, i.e., to a weakening of interface scattering for alloyed SLs. The calculations also allow us to address finite‐thickness effects on the measured thermal conductivity data. Although the used SL had a total thickness of only ∼250 nm, its thermal conductivity can be assumed to coincide with that of a “bulk” (infinitely thick) SL prior to annealing. As interdiffusion increases, boundary scattering at the film/substrate interface becomes relevant and leads to a slow increase of κ. Besides its fundamental relevance, this work shows that the thermal stability of superlattices is limited, and that sizeable structural changes (including defect formation) occur already at operation temperatures of ∼650 °C.