# Tuneable superconducting effective gap in graphene-TMDC heterostructures

## TL;DR

This paper investigates how the effective superconducting gap in graphene-TMDC heterostructures can be tuned by various parameters, revealing the influence of spin-orbit coupling and pairing symmetry on superconducting excitations.

## Contribution

It introduces a formalism for the low-energy Hamiltonian of graphene-TMDC heterostructures with superconductivity, highlighting the effects of key parameters on the superconducting gap and excitations.

## Key findings

- Superconducting excitations are significantly affected by spin-orbit coupling parameters.
- Spin triplet p-wave pairing increases the subgap energy compared to s-wave.
- Dependence of superconducting energy on chemical potential is characterized.

## Abstract

Growth of graphene on monolayer transition-metal dichalcogenides presents opening on band gap and giant spin-orbit coupling which paves the way to achieve a useful hybrid structure for electronics and spintronics applications. Increase of the atomic number of transition-metal results in a large SOC, where eventually a band inversion appears in graphene-$WSe_2$. We consider superconductor induction by proximity effect to the graphene-TMDC hybrid structure. As a necessity of formalism, we introduce a proper time-reversal and particle-hole symmetry operators, under which the $8 \times 8$ Dirac-Bogoliubov-de Gennes low-energy effective Hamiltonian is invariant. Resulting superconducting electron-hole excitations shows that, the essential dynamical parameters $\lambda_I^{A,B}$ and $\lambda_R$ have significant effect on superconducting excitations and, specifically, subgap energy. Dependence of the superconducting energy excitation on chemical potential is explored. The signature of spin triplet $p$-wave pairing symmetry in the system is found to increase the subgap superconducting energy, in comparing to $s$-wave symmetry.