Abstract

The resistance as a function of tip-sample separation in the scanning tunneling microscope is calculated for distances in the transition region between tunneling and point contact. A resistance plateau appears near point contact with value $\frac{A\ensuremath{\pi}\ensuremath{\hbar}}{{e}^{2}}$, where $A$ is of order unity, its exact value depending on the identity of the tip atom. Good agreement is found with the recent experimental data of Gimzewski and M\oller.

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