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Electron beam induced deposition of low resistivity platinum from Pt(PF3)(4)

机译:电子束诱导从Pt(PF3)(4)沉积低电阻率铂

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The authors have deposited Pt from Pt(PF3)(4) using a focused 10 keV electron beam (scanning electron microscopy) in an FEI 620 dual beam system and measured the resistivity and composition of the deposits. To measure resistivity, lines of Pt were deposited across four gold fingers and the cross-sectional area of the lines was measured by focused ion beam sectioning. The resistivity varies between about 30 and 650 mu Omega cm and is orders of magnitude lower than the resistivity achieved by e-beam-induced deposition using the usual organometallic precursor, (methylcyclopentadienyl) trimethyl platinum. In general, the higher the beam current the lower the resistivity. They have used wavelength dispersive x-ray analysis to measure the composition of rectangles deposited with various beam currents. Typical at.% values of (Pt:P:F) are 81:17:2 and 58:32:10. Minimum linewidth that they have deposited is 80 nm, and with a stationary beam of 2.8 nA they have deposited a pillar of 135 nm in diameter. They have also deposited Pt structures on freestanding carbon nanotubes and have used the deposits to contact nanofibers. Electron-beam-induced deposition of a "good" metal is particularly useful in geometries where standard lithography is awkward, such as making contacts to fibers or nanotubes randomly dispersed on a surface or freestanding. (c) 2006 American Vacuum Society.
机译:作者在FEI 620双电子束系统中使用聚焦的10 keV电子束(扫描电子显微镜)从Pt(PF3)(4)沉积了Pt,并测量了电阻率和沉积物的成分。为了测量电阻率,在四个金手指上沉积了Pt线,并通过聚焦离子束切片测量了线的横截面积。电阻率在大约30至650μOΩcm之间变化,并且比使用常规有机金属前体(甲基环戊二烯基)三甲基铂的电子束诱导沉积所获得的电阻率低几个数量级。通常,电子束电流越高,电阻率越低。他们使用波长色散X射线分析来测量沉积有各种束流的矩形的组成。 (Pt:P:F)的典型at。%值为81:17:2和58:32:10。它们沉积的最小线宽为80 nm,并且在2.8 nA的固定光束下,它们沉积的直径为135 nm的柱。他们还在独立的碳纳米管上沉积了Pt结构,并使用沉积物来接触纳米纤维。电子束诱导的“良好”金属的沉积在标准光刻难以处理的几何结构中(例如与随机分散在表面或独立的纤维或纳米管的接触中)特别有用。 (c)2006年美国真空学会。

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