Abstract

Recently, unconventional superconductivity having a zero-bias conductance peak is reported in doped topological Dirac semimetal (DSM) with lattice distortion. Motivated by the experiments, we theoretically study the possible symmetry-lowering lattice distortions and their effects on the emergence of unconventional superconductivity in doped topological DSM. We find four types of symmetry-lowering lattice distortions that reproduce the crystal symmetries relevant to experiments from the group-theoretical analysis. Considering inter-orbital and intra-orbital electron density-density interactions, we calculate superconducting phase diagrams. We find that the lattice distortions can induce unconventional superconductivity hosting gapless surface Andreev bound states (SABS). Depending on the lattice distortions and superconducting pairing interactions, the unconventional inversion-odd-parity superconductivity can be either topological nodal superconductivity hosting a flat SABS or topological crystalline superconductivity hosting a gapless SABS. Remarkably, the lattice distortions increase the superconducting critical temperature, which is consistent with the experiments. Our work opens a pathway to explore and control pressure-induced topological superconductivity in doped topological semimetals.

Highlights

  • Because all bands are doubly degenerate due to the time-reversal symmetry (TRS) and inversion symmetry (IS), a Dirac semimetal (DSM) is minimally described by a four-band H­ amiltonian6,10,38–40

  • We have studied the possible symmetry-lowering lattice distortions and their effects on the emergence of unconventional superconductivity in doped topological DSM

  • We investigated the possible superconductivity under such symmetry-lowering lattice distortions considering inter-orbital and intra-orbital electron density-density interactions

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Summary

Methods

To study the effects of symmetry-lowering lattice distortions, we assume a minimal 4 × 4 Hamiltonian that describes representative topological Dirac ­semimetals, where the lattice distortions are implemented as a ­perturbation. We construct the Bogoliubov-de Gennes (BdG) Hamiltonian within the mean-field approximation while keeping TRS and the crystal ­symmetry. The momentum independent pairing potentials are classified using irreducible representations of the unbroken point ­group. The nodal structures, chiral winding number in Eq [43], and chiral mirror winding number in Eq [47] are calculated using the BdG Hamiltonian. The surface Green’s functions are calculated using a Möbius transformationbased ­method. The superconducting critical temperature Tc is calculated by solving the linearized gap equation in the weak-coupling l­imit. All the details are provided in the main text and Supplementary Information

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