Abstract
The group-IV alloy semiconductors, including C, Si, Ge, and Sn, have been actively investigated for use in heterojunction devices compatible with Si circuit technology [1,2]. For a variety of technical reasons, in particular to adjust the strain in the het-eroepitaxial layers, it is desirable to adjust the stain in the group-IV materials and form alloys (e.g., Si1-x C x , and Si1-x-y Ge x C y ). For the Si-Ge system, the bond-length mismatch is only 4%, whereas it is about 40% for the Si-C system. Due to the small covalent radius of the C atom, the incorporation of C in substitutional sites can lead to the strain relaxation of compressively strained Si-Ge alloy. According to Vegard’s law, the lattice-matching condition for Si1-x-y Ge x C y on Si is x=8.2y (Si1-9.2yGe8i2yCy) [2]. It must be noted, however, that the solid solubilities of C in these constituents are extremely low (∼3×1018 cm-3 for Si and ∼5×1018 cm-3 for Ge at the melting points [3]). Growth under nonequilibrium conditions at relatively low growth temperatures enables us to obtain alloys with significant C fractions. Indeed, Si1-x C x alloys with C fractions as high as x∼0.2 have been prepared by MBE, and Si1-x-y Ge x C y alloys with y≤0.1 have been achieved by CVD (see Ref. [4]).
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Adachi, S. (1999). Carbon-Incorporated Alloys (SI1-x C x , SI1-x-y GE x C y , etc.). In: Optical Constants of Crystalline and Amorphous Semiconductors. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-5247-5_10
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DOI: https://doi.org/10.1007/978-1-4615-5247-5_10
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