Conducting Atomic Force Microscopy Studies of Nanoscale Cobalt Silicide Schottky Barriers on Si(111) and Si(100)

TL;DR

This study uses conducting atomic force microscopy to analyze nanoscale cobalt silicide Schottky barriers on silicon substrates, revealing effects of surface passivation, impurities, and temperature on barrier properties.

Contribution

It provides detailed measurements of Schottky barrier heights and ideality factors on passivated and non-passivated silicon surfaces, highlighting the influence of surface states and impurities.

Findings

Non-passivated surfaces lower barrier heights by 0.2-0.3 eV due to Fermi level pinning.

Barrier heights are similar on Si(111) and Si(100), indicating impurity effects.

Barrier heights decrease and ideality factors increase with decreasing temperature.

Abstract

Cobalt silicide (CoSi2) islands have been formed by the deposition of thin films (~0.1 to 0.3 nm) of cobalt on clean Si(111) and Si(100) substrates in ultrahigh vacuum (UHV) followed by annealing to ~880 degrees C. Conducting atomic force microscopy has been performed on these islands to characterize and measure their current-voltage (I-V) characteristics. Current-voltage curves were analyzed using thermionic emission theory to obtain the Schottky barrier heights and ideality factors between the silicide islands and the silicon substrates. Current-voltage measurements were performed ex situ for samples ("passivated surfaces") where the silicon surface surrounding the islands was passivated with a native oxide. Other samples ("clean surfaces") remained in UHV while I-V curves were recorded. By comparing barrier heights and ideality factors for islands on both surfaces, the effects of the non-passivated surfaces on conduction were studied. The clean surface barrier heights were found to be ~0.2 to 0.3 eV below barrier heights measured from similar islands on passivated surfaces. The reduced Schottky barrier is mainly attributed to Fermi level pinning by non-passivated surface states of the clean silicon surface. However, the measured barrier heights of the clean surface islands are equivalent on both Si(111) and Si(100), suggesting that the non-passivated surfaces are influenced by cobalt impurities. Furthermore, the barrier heights of islands on the clean surfaces are lower than due to Fermi level pinning alone and the additional barrier height lowering is primarily attributed to spreading resistance effects. Schottky barrier inhomogeneity may also cause additional barrier height lowering and non-ideality in the contacts. The clean surface barrier heights decreased and the ideality factors increased with decreasing temperature, which is attributed to the temperature variation of the Fermi level.