About Milap Singh

Solid State Physics Laboratory
Defence R&D Organization
Lucknow Road, Timarpur,
Delhi-110054, India
Email: milap.singh@sspl.drdo.in

He received his B.Sc. Physics degree from University of Delhi, India in 2004 and M.Sc. Physics degree from University of Delhi, India in 2007. He worked as Assistant Professor in ARSD College, University of Delhi (2008-2009) and joined Solid State Physics Laboratory, Def. Res. & Dev. Orgn. in 2009. He is currently working as a scientist in MEMS Technology Group. His main research interests are in the field of Gold Electroplating for MEMS applications, Photolithography, Thin dielectric film deposition and Stress studies in thin films.

An improved analytical method for reducing edge built up and estimation of thickness in selective plating using variable perimeter-to-area ratio window test mask

In this paper, we attempt to present a new approach and analytical relation between perimeter-to-area ratio (P/A) and the plated thickness using Variable Area Window (VAW) test mask for improved thickness estimation. Although, the approach is illustrated using selective plating of gold films by varying two dimensional patterned windows on metallised silicon surface as an example, yet the method can be applied to other cases also. The method includes selective electroplating of gold in rectangular and circular windows wherein P/A of patterned shapes (squares, rectangles and circles) has been varied from 0.001 cm-1 to 0.4 cm-1 i.e. a factor of 400, a range normally used for practical modern MEMS devices. Experiments show that in general the thickness increases with increasing P/A because of current crowding. However, in contrast to using current density for control of this current crowding as reported in literature, we report that by careful design of mask pattern and improved material parameters, one can control and even achieve a slope reversal in the plot of thickness vs. P/A. The increase in thickness as measured by slope of linear fit is about 3 µm/(P/A in µm-1) for sharp edges compared to about 0.8 µm/(P/A in µm-1) for curved edges within the experimental errors. The general applicability of these relations to practical cases is confirmed by analysing the previously reported trends of data from the literature on Ni films using similar patterned shapes.