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Experimental And Simulation Studies Of Resistivity In Nanoscale Copper Films

机译:纳米铜膜电阻率的实验与模拟研究

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The effect of film thickness on the resistivity of thin, evaporated copper films (approximately 10-150 nm thick) was determined from sheet resistance, film thickness, and mean grain-size measurements by using four-point probe, profilometer, and electron backscatter diffraction (EBSD) and X-ray diffraction (XRD) methods, respectively. The resistivity of these films increased with decreasing film thickness in a manner that agreed well with the dependence given by a versatile simulation program, published earlier, using the measured values for the mean grain size and fitting parameters for surface and grain boundary scattering. Measurements of the change in sheet resistance with temperature of these films and the known change in resistivity with temperature for pure, bulk copper were used to calculate the thickness of these films electrically by using Matthiessen's rule (this is often referred to as an "electrical thickness"). These values agreed to within 3 nm of those obtained physically with the profilometer. Hence, Matthiessen's rule can continue to be used to measure the thickness of a copper film and, by inference, the cross-sectional area of a copper line for dimensions well below the mean free path of electrons in copper at room temperature (39 nm).
机译:薄膜厚度对蒸发的薄铜薄膜(约10-150 nm厚)的电阻率的影响是通过使用四点探针,轮廓仪和电子背散射衍射从薄层电阻,薄膜厚度和平均粒度测量中确定的(EBSD)和X射线衍射(XRD)方法。这些膜的电阻率随着膜厚的减小而增加,其方式与之前发布的通用模拟程序给出的依赖性很好地吻合,该程序使用平均晶粒尺寸的测量值以及表面和晶界散射的拟合参数。这些薄膜的表面电阻随温度的变化以及已知的纯铜块体电阻随温度的变化的测量结果通过使用Matthiessen法则(通常称为“电气厚度”)以电学方式计算这些膜的厚度。 ”)。这些值与轮廓仪实际获得的值相差3 nm之内。因此,可以继续使用Matthiessen法则来测量铜膜的厚度,并据此推断铜线的横截面积,其尺寸远低于室温(39 nm)下铜中电子的平均自由程。 。

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