Inverse proximity effect in s -wave and d -wave superconductors coupled to topological insulators

• Published in: Physical review. B 2019-03, Vol.99 (9), p.094505, Article 094505
• Main Authors: Hugdal, Henning G., Amundsen, Morten, Linder, Jacob, Sudbø, Asle
• Format: Article
• Language: English
• Subjects: Chemical potential; Cuprates; Fermions; Green's functions; Order parameters; Organic chemistry; Proximity; Proximity effect (electricity); Spin-orbit interactions; Superconductivity; Topological insulators; Topology
• ISSN: 2469-9950; 2469-9969
• DOI: 10.1103/PhysRevB.99.094505

We study the inverse proximity effect in a bilayer consisting of a thin s- or d-wave superconductor (S) and a topological insulator (TI). Integrating out the topological fermions of the TI, we find that spin-orbit coupling is induced in the S, which leads to spin-triplet p-wave (f-wave) correlations in the anomalous Green's function for an s-wave (d-wave) superconductor. Solving the self-consistency equation for the superconducting order parameter, we find that the inverse proximity effect can be strong for parameters for which the Fermi momenta of the S and TI coincide. The suppression of the gap is approximately proportional to e−1/λ, where λ is the dimensionless superconducting coupling constant. This is consistent with the fact that a higher λ gives a more robust superconducting state. For an s-wave S, the interval of TI chemical potentials for which the suppression of the gap is strong is centered at μTI=±2mvF2μA2, and increases quadratically with the hopping parameter t. Since the S chemical potential μ typically is high for conventional superconductors, the inverse proximity effect is negligible except for t above a critical value. For sufficiently low t, however, the inverse proximity effect is negligible, in agreement with what has thus far been assumed in most works studying the proximity effect in S-TI structures. In superconductors with low Fermi energies, such as high-Tc cuprates with d-wave symmetry, we again find a suppression of the order parameter. However, since μ is much smaller in this case, a strong inverse proximity effect can occur at μTI=0 for much lower values of t. Moreover, the onset of a strong inverse proximity effect is preceded by an increase in the order parameter, allowing the gap to be tuned by several orders of magnitude by small variations in μTI.