Two-band superconductivity of bulk and surface states in Ag thin films on Nb

Abstract

We use epitaxial strain to shift the energy of the two-dimensional Ag(111) surface states of Ag islands on Nb(110) substrates, allowing to spatially tune the bottom of the surface-state band $E_{\mathrm{SS}}$ through the Fermi level $E_{\mathrm{F}}$. Bulk and surface-state contributions to the Ag(111) local density of states (LDOS) can be separated with scanning tunneling spectroscopy. For thick islands ($\approx$\, 20 nm), the Ag surface states are decoupled from the Ag bulk states via orthogonality, and the superconductive gap induced by proximity to Nb is due to bulk states only. However, for thin islands (3-4 nm), surface-state electrons develop superconducting correlations as identified by a complete energy gap in the LDOS when $E_{\mathrm{F}}$ is smaller than but close to $E_{\mathrm{F}}$. The induced superconductivity in this case is of two-band nature and appears to occur when the surface-state wave function reaches down to the Ag/Nb interface.

5 pages, 4 figures

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• Quantum Spin Hall Insulator State in HgTe Quantum Wells
• Superconducting proximity effect and Majorana fermions at the surface of a topological insulator
• Phase controlled superconducting proximity effect probed by tunneling spectroscopy
• Electrostatically Induced Superconductivity at the Surface of WS${}_2$
• Revealing surface states in In-doped SnTe superconducting nanoplates with low bulk mobility

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