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Title: Inverse modeling applied to Scanning Capacitance Microscopy for improved spatial resolution and accuracy

Journal Article · · AIP Conference Proceedings
DOI:https://doi.org/10.1063/1.56917· OSTI ID:21202330
;  [1]
  1. Department of Physics, University of Utah, Salt Lake City, Utah 84112 (United States)

Scanning Capacitance Microscopy (SCM) is capable of providing two-dimensional information about dopant and carrier concentrations in semiconducting devices. This information can be used to calibrate models used in the simulation of these devices prior to manufacturing and to develop and optimize the manufacturing processes. To provide information for future generations of devices, ultra-high spatial accuracy (<10 nm) will be required. One method, which potentially provides a means to obtain these goals, is inverse modeling of SCM data. Current semiconducting devices have large dopant gradients. As a consequence, the capacitance probe signal represents an average over the local dopant gradient. Conversion of the SCM signal to dopant density has previously been accomplished with a physical model which assumes that no dopant gradient exists in the sampling area of the tip. The conversion of data using this model produces results for abrupt profiles which do not have adequate resolution and accuracy. A new inverse model and iterative method has been developed to obtain higher resolution and accuracy from the same SCM data. This model has been used to simulate the capacitance signal obtained from one and two-dimensional ideal abrupt profiles. This simulated data has been input to a new iterative conversion algorithm, which has recovered the original profiles in both one and two dimensions. In addition, it is found that the shape of the tip can significantly impact resolution. Currently SCM tips are found to degrade very rapidly. Initially the apex of the tip is approximately hemispherical, but quickly becomes flat. This flat region often has a radius of about the original hemispherical radius. This change in geometry causes the silicon directly under the disk to be sampled with approximately equal weight. In contrast, a hemispherical geometry samples most strongly the silicon centered under the SCM tip and falls off quickly with distance from the tip's apex. Simulation of the expected signal for each tip geometry shows significant differences in the expected resolution. This has also been explored experimentally with the SEMATECH no.1 sample. This sample has a staircase dopant profile with 50 nm steps. Simulation of the expected signal for the SEMATECH No.1 using a flat tip model shows good agreement with measured data. However, the flattened tip reduces the steps in the profile to inflections.

OSTI ID:
21202330
Journal Information:
AIP Conference Proceedings, Vol. 449, Issue 1; Conference: 1998 international conference on characterization and metrology for ULSI technology, Gaithersburg, MD (United States), 23-27 Mar 1998; Other Information: DOI: 10.1063/1.56917; (c) 1998 American Institute of Physics; Country of input: International Atomic Energy Agency (IAEA); ISSN 0094-243X
Country of Publication:
United States
Language:
English