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Probing resistivity and doping concentration of semiconductors at the nanoscale using scanning microwave microscopy

机译:探测电阻率和掺杂浓度使用扫描半导体在纳米尺度上微波显微镜

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摘要

We present a new method to extract resistivity and doping concentration of semiconductor materials from Scanning Microwave Microscopy (SMM) S-11 reflection measurements. Using a three error parameters de-embedding workflow, the S-11 raw data are converted into calibrated capacitance and resistance images where no calibration sample is required. The SMM capacitance and resistance values were measured at 18 GHz and ranged from 0 to 100 aF and from 0 to 1 M Omega, respectively. A tip-sample analytical model that includes tip radius, microwave penetration skin depth, and semiconductor depletion layer width has been applied to extract resistivity and doping concentration from the calibrated SMM resistance. The method has been tested on two doped silicon samples and in both cases the resistivity and doping concentration are in quantitative agreement with the data-sheet values over a range of 10(-3) Omega cm to 10(1) Omega cm, and 10(14) atoms per cm(3) to 10(20) atoms per cm(3), respectively. The measured dopant density values, with related uncertainties, are [1.1 +/- 0.6] x 10(18) atoms per cm3, [2.2 +/- 0.4] x 10(17) atoms per cm(3), [4.5 +/- 0.2] x 10(16) atoms per cm(3), [4.5 +/- 1.3] x 10(15) atoms per cm3, [4.5 +/- 1.7] x 10(14) atoms per cm(3). The method does not require sample treatment like cleavage and cross-sectioning, and high contact imaging forces are not necessary, thus it is easily applicable to various semiconductor and materials science investigations.
机译:我们提出一种新的方法来提取电阻率半导体材料的掺杂浓度从微波扫描显微镜S-11模式反射测量。参数de-embedding工作流,S-11生数据转换成校准电容和抵抗图像没有校准样品是必需的。测量值在18个GHz范围从0到100年房颤和从0到1 Mω,分别。tip-sample分析模型,包括小费半径,微波穿透皮肤深度和半导体耗尽层宽度应用于提取电阻率和兴奋剂多发性骨髓瘤浓度校准的阻力。两种掺杂硅的方法测试在这两种情况下,电阻率和样本掺杂浓度的定量协议与数据手册值范围10(3)ω厘米到10(1)ω厘米,和10 (14)原子每厘米(3)到10(20)的原子/厘米(3),分别。与相关的不确定性,是1.1 + / - 0.6 x10(18)原子每立方厘米(2.2 + / - 0.4)x 10 (17)(3)原子每厘米,(4.5 + / - 0.2)x 10(16)的原子/厘米(3),(4.5 + / - 1.3)x 10(15)原子每立方厘米(4.5+ / - 1.7) * 10(14)的原子/厘米(3)。不需要样品处理喜欢乳沟吗和浆纱切片,高接触成像部队并不是必要的,因此它很容易适用于各种半导体材料科学调查。

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