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

被引:43
作者
Barry, John D. [1 ]
Ervin, Matthew [2 ]
Molstad, Jay [2 ]
Wickenden, Alma [2 ]
Brintlinger, Todd [1 ,2 ]
Hoffman, Patrik [1 ,3 ]
Melngailis, John [1 ]
机构
[1] Univ Maryland, Inst Res Elect & Appl Phys, College Pk, MD 20742 USA
[2] USA, Res Lab, AMSRD, ARL,SE,RL, Adelphi, MD 20783 USA
[3] Ecole Polytech Fed Lausanne, Adv Photon Lab, CH-1015 Lausanne, Switzerland
来源
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B | 2006年 / 24卷 / 06期
关键词
D O I
10.1116/1.2395962
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
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.
引用
收藏
页码:3165 / 3168
页数:4
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