首页> 外文期刊>Journal of Crystal Growth >Characterization of interface roughness scattering of electrons in an In_(0.53)Ga_(0.47)As/In_(0.52)Al_(0.48)As QW-HEMT structure with (411)A super-flat interfaces
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Characterization of interface roughness scattering of electrons in an In_(0.53)Ga_(0.47)As/In_(0.52)Al_(0.48)As QW-HEMT structure with (411)A super-flat interfaces

机译:具有(411)A超平界面的In_(0.53)Ga_(0.47)As / In_(0.52)Al_(0.48)As QW-HEMT结构中电子的界面粗糙度散射的表征

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摘要

In order to characterize interface roughness scattering, two-dimensional electron gas (2DEG) mobility in (411)A and (100) selectively-doped In_(0.53)Ga_(0.47)As/In_(0.52)Al_(0.48)As quantum well (QW) HEMT structures, which were grown on InP substrates by molecular beam epitaxy, with a gate contact was measured at 20 K as a function of sheet electron concentration (N_s) by changing gate bias. Thickness of the QW was designed to be rather small (6 nm) for enhancing the interface roughness scattering for both samples. 2DEG mobilities of the (411)A sample were 21,000-51, 400 cm~2/V s in the range of N_s = 0.7-1.7 x 10~(12) cm~(-2), which are about more than 2 times higher than the mobilities (8,700-25,400 cm~2 /V s) of the conventional (100) sample, 2DEG mobility was calculated by taking into account interface roughness scattering and ionized remote impurity scattering. By fitting the calculated results to the observed ones, lateral size (Λ) and height (Δ) of the interface roughness of the (411)A sample were determined to be 3.5 and 0.23 nm, respectively, which are 30% and 50% smaller than the corresponding values (Λ = 5.0 nm and Δ = 0.43 nm) of the (100) sample.
机译:为了表征界面粗糙度散射,在(411)A和(100)中二维掺杂In_(0.53)Ga_(0.47)As / In_(0.52)Al_(0.48)As量子阱中的二维电子气(2DEG)迁移率(QW)通过分子束外延在InP衬底上生长的具有栅极接触的(HEW)HEMT结构在20 K时通过改变栅极偏置量作为薄层电子浓度(N_s)的函数进行测量。 QW的厚度设计得很小(6 nm),以增强两个样品的界面粗糙度散射。 (411)A样品的2DEG迁移率是21,000-51,400 cm〜2 / V s在N_s = 0.7-1.7 x 10〜(12)cm〜(-2)的范围内,约为2倍以上比常规(100)样品的迁移率(8,700-25,400 cm〜2 / V s)高,通过考虑界面粗糙度散射和电离远程杂质散射来计算2DEG迁移率。通过将计算结果拟合到观察到的结果,确定(411)A样品的界面粗糙度的横向尺寸(Λ)和高度(Δ)分别为3.5和0.23 nm,分别小30%和50%比(100)样品的相应值(Λ= 5.0 nm和Δ= 0.43 nm)。

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