PbTe HWE薄膜的霍尔迁移率和场效应迁移率研究

P.R. Vaya , J. Majhi , B.S.V. Gopalam , C. Dattatreyan
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引用次数: 1

摘要

采用热壁外延(HWE)技术对KCl(100)衬底上不同厚度的PbTe薄膜的霍尔迁移率(μH)和场效应迁移率(μFE)进行了研究。采用标准的范德保技术获得了霍尔迁移率。计算了由于尺寸效应引起的扩散散射迁移率μD,并与μH进行了比较。μH和μD之间存在较大差异的原因是由于晶界、位错、解理步骤和其他表面效应引起的散射导致了残余迁移率的贡献。对于交流电场效应的研究,采用了一种MIS结构,在薄膜表面和金属电极之间有一层薄云母间隔层。在温度为98 ~ 156 K,频率为40 ~ 200 kHz的范围内,获得了不同温度下的场效应迁移率μFE。μFE随频率的变化主要是由于在上述温度范围内具有时间常数为1.84 ~ 0.96 μs的快表面态的弛豫。这些表面态的活化能和俘获截面分别为0.02 eV和10−19 cm2。与霍尔迁移率不同,由实验结果得出的有效直流场效应迁移率与薄膜厚度无关。
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Hall mobility and field effect mobility studies on PbTe HWE thin films

Hall mobility (μH) and field effect mobility (μFE) studies were carried out on PbTe films of different thickness grown on KCl (100) substrates by the hot wall epitaxy (HWE) technique. The Hall mobility was obtained using the standard Van der Pauw technique. The diffused scattering mobility, μD, due to size effect was calculated and compared with μH. A large discrepancy between μH and μD was explained on the basis of a residual mobility contribution which was attributed to the scattering due to grain boundaries, dislocations, cleavage steps and other surface effects. For AC field effect studies an MIS structure with a thin mica spacer between the film surface and metal electrode was used. The field effect mobility, μFE, was obtained at different temperatures from 98 to 156 K in the frequency range of 40 to 200 kHz. The variation of μFE with frequency was found to be largely due to the relaxation of fast surface states having time constants from 1.84 to 0.96 μs in the above temperature range. The activation energy and capture cross-section of these surface states were calculated to be 0.02 eV and 10−19 cm2 respectively. Unlike the Hall mobility, the effective DC field effect mobility derived from the experimental results was found to be independent of film thickness.

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