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We self-consistently solve the Bogoliubov–de Gennes equations on the tight-binding model for s-wave topological superconductivity (TSC) in two-dimensional (2D) quasicrystals (QCs). For the mean fields, we consider not only the superconducting order parameter but also the spin-dependent Hartree potential. We calculate the topological invariant for 2D Ammann–Beenker (AB) QCs to examine the realization of TSC in QCs. We demonstrate TSC in QCs whose distribution of the superconducting order parameter reflects the symmetry of the structure of AB QCs. Furthermore, we perform momentum-space analysis by calculating the spectral function. We identify specific wave numbers which are to be related to the topological phase transition in AB QCs.

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