Turning non-superconducting elements into superconductors by quantum confinement and proximity

Elemental good metals, including noble metals (Cu, Ag, Au) and several s-block elements, do not exhibit superconductivity in bulk at ambient pressure, primarily due to weak electron--phonon coupling that fails to overcome Coulomb repulsion. In this perspective, we examine whether quantum confinement alone, or in combination with proximity effects, can induce an observable superconducting instability in metals that are non-superconducting in bulk form. We review recent theoretical progress and present a unified framework based on a confinement-generalized, isotropic one-band Eliashberg theory, in which the normal density of states becomes energy dependent and key material parameters $E_F$, $λ$, and $μ^*$ acquire an explicit thickness dependence. By numerically solving the resulting Eliashberg equations using ab-initio or experimentally determined electron--phonon spectral functions α²F(Ω) and Coulomb pseudopotentials μ^*, and without introducing adjustable parameters, we compute the critical temperature T_c as a function of film thickness for representative noble, alkali, and alkaline-earth metals. The theory predicts that superconductivity can emerge only in selected cases and within extremely narrow thickness windows, typically centered around sub-nanometer scales $L sim 0.4$--$0.6$ nm. We further discuss layered superconductor/normal-metal systems, where quantum confinement and proximity effects coexist. In these heterostructures, a substantial enhancement of the critical temperature is predicted, even when the constituent materials are non-superconducting or poor superconductors in bulk form.