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首页> 外文期刊>Journal of Superconductivity and Novel Magnetism >Manifestation of the Transition Semiconductor-Semimetal and Intrinsic Interface State in Band Structure and Magneto-Transport Properties in Nanostructure Superlattice
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Manifestation of the Transition Semiconductor-Semimetal and Intrinsic Interface State in Band Structure and Magneto-Transport Properties in Nanostructure Superlattice

机译:过渡态半导体-半金属和本征界面态在能带结构中的表现以及纳米结构超晶格中的磁输运性质

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摘要

We report here G carrier's magneto-transport properties and the band structure results for II-VI semiconductors. HgTe is a zero gap semiconductor and when it is sandwiched between CdTe layers yield a small gap HgTe/CdTe superlattice which is the key to development of an infrared detector. Our sample, grown by MBE, had a period d (100 layers) of 18 nm (HgTe)/4.4 nm (CdTe). Calculations of the spectra of energy E(k_z) and E(k_p), respectively, in the direction of growth and in the plane of the superlattice were performed in the envelope-function formalism. The angular dependence of the transverse magnetoresistance follows the two-dimensional (2D) behavior with Shubnikov-de Haas oscillations. At low temperature, the sample exhibits p-type conductivity with a hole mobility of 900 cm~2/V·s. A reversal of the sign of the weak-field Hall coefficient occurs at 25 K with an electron mobility of 3 × 10~4 cm~2/V·s. In the intrinsic regime, the measured E_g ≈ 38 meV agrees with the calculated E_g(Γ, 300 K) = 34 meV, which coincide with the Fermi level energy. The formalism used here predicts that this narrow gap sample is semi-metallic, quasi-two-dimensional and far-infrared detector.
机译:我们在此报告G载流子的磁传输特性和II-VI半导体的能带结构结果。 HgTe是零间隙半导体,当其夹在CdTe层之间时,会产生小间隙的HgTe / CdTe超晶格,这是开发红外探测器的关键。通过MBE生长的我们的样品的周期d(100层)为18 nm(HgTe)/4.4 nm(CdTe)。在包络函数形式中分别计算了能量E(k_z)和E(k_p)在生长方向和超晶格平面内的光谱。横向磁阻的角度依赖性遵循Shubnikov-de Haas振荡的二维(2D)行为。在低温下,样品表现出p型电导率,空穴迁移率为900 cm〜2 / V·s。弱电场霍尔系数的符号在25 K时发生,电子迁移率为3×10〜4 cm〜2 / V·s。在本征状态下,测得的E_g≈38 meV与计算出的E_g(Γ,300 K)= 34 meV一致,这与费米能级一致。此处使用的形式主义预测该窄间隙样品是半金属,准二维和远红外检测器。

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