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Si-Ge interdiffusion in strained Si/strained SiGe heterostructures and implications for enhanced mobility metal-oxide-semiconductor field-effect transistors

机译:应变硅/应变硅锗异质结构中的硅锗互扩散及其对提高迁移率的金属氧化物半导体场效应晶体管的影响

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摘要

Si-Ge interdiffusivity in epitaxial strained Si/Si_(1-y)Ge_y/strained Si/relaxed Si_(1-x0)Ge_(x0) heterostructures is extracted for Ge fractions between 0 and 0.56 over the temperature range of 770-920 ℃. Boltzmann-Matano analysis is applied to determine interdiffusivity from diffused Ge profiles in strained Si/relaxed Si_(1-x0)Ge_(x0) heterostructures [L. Boltzmann, Wiedemanns Ann. Phys. 53, 959 (1894) and C. Matano, Jpn. J. Phys. 8, 109 (1933)]. A model for the interdiffusivity suitable for use in the process simulator TSUPREM-4 is constructed. Si-Ge interdiffusivity increases by 2.2 times for every 10% increase in Ge fraction for interdiffusion in strained Si/relaxed Si_(1-x0)Ge_(x0) samples. Significantly enhanced Si-Ge interdiffusion is observed for Si_(1-y)Ge_y layers under biaxial compressive strain. Si-Ge interdiffusivity is found to increase by 4.4 times for every 0.42% increase in the magnitude of biaxial compressive strain in the Si_(1-y)Ge_y, which is equivalent to a decrease in the Ge percentage in the substrate by 10 at. %. These results are incorporated into an interdiffusion model that successfully predicts experimental interdiffusion in various SiGe heterostructures. The extracted activation energy and prefactor for the interdiffusivity are 4.66 eV and 310 cm~2/s, respectively, for the temperature and Ge fraction ranges of this study. Threading dislocation densities on the order of 10~7 cm~(-2) are shown to have negligible effect on Si-Ge interdiffusion in Si/Si_(0.69)Ge_(0.31) structures. Substituting the strained Si layers surrounding the Si_(1-y)Ge_y peak layer with SiGe layers is shown to have little effect on the Si-Ge interdiffusivity. The implications of these findings for the design and process integration of enhanced mobility strained Si/strained SiGe metal-oxide-semiconductor field-effect transistors are discussed.
机译:在770-920℃的温度范围内,提取了0〜0.56之间的Ge分数的外延应变Si / Si_(1-y)Ge_y /应变Si /松弛Si_(1-x0)Ge_(x0)异质结构中的Si-Ge互扩散性。 。 Boltzmann-Matano分析用于确定应变Si /松弛Si_(1-x0)Ge_(x0)异质结构[L.玻尔兹曼,韦德曼·安物理53,959(1894)和C. Matano,Jpn。 J.物理8,109(1933)]。构建适用于过程模拟器TSUPREM-4的互扩散模型。对于在应变Si /松弛Si_(1-x0)Ge_(x0)样品中进行互扩散,Ge分数每增加10%,Si-Ge互扩散性就会提高2.2倍。在双轴压缩应变下,Si_(1-y)Ge_y层的Si-Ge相互扩散显着增强。发现Si_(1-y)Ge_y中双轴压缩应变的幅度每增加0.42%,Si-Ge互扩散性就会增加4.4倍,这相当于基板中Ge的百分比降低10 at。 %。这些结果被并入到互扩散模型中,该模型成功地预测了各种SiGe异质结构中的实验互扩散。在本研究的温度和Ge分数范围内,提取的活化能和互扩散系数分别为4.66 eV和310 cm〜2 / s。结果表明,在Si / Si_(0.69)Ge_(0.31)结构中,螺纹位错密度对Si-Ge互扩散的影响可忽略不计,约为10〜7 cm〜(-2)。用SiGe层代替围绕Si_(1-y)Ge_y峰层的应变Si层对Si-Ge互扩散性影响很小。讨论了这些发现对增强迁移率应变Si /应变SiGe金属氧化物半导体场效应晶体管的设计和工艺集成的影响。

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