We study the superconducting pairing symmetry in twisted bilayer graphene by solving the Bogoliubov-de Gennes equation for all electrons in moir'{e} supercells. With increasing the pairing potential, the system evolves from the mixed nontopological and phase to the phase via the first-order phase transition. In the time-reversal symmetry breaking and phase, vortex and antivortex lattices accompanying spontaneous supercurrent are induced by the twist. The superconducting order parameter is nonuniform in the moir'{e} unit cell. Nevertheless, the superconducting gap in the local density of states is identical in the unit cell. The twist-induced vortices and nontopological nature of the mixed and phase are not captured by the existing effective models. Our results suggest the importance of long-range pairing interaction for effective models.

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