Topological superconductivity in superconducting chiral topological semimetals with parallel spin-momentum locking

Distinguished from conventional band-inversion-induced Weyl semimetals, chiral topological semimetals host helicoid-arc surface states originating from time-reversal invariant momenta of the Brillouin zone. Motivated by the experimental observation of parallel spin-momentum locking in chiral topological semimetals, we find that parallel spin-momentum locking leads to helicoid-arc surface states. We also investigate the potential intrinsic topological phases in a superconducting chiral topological semimetal with s_±- wave pairing. We find that a first-order time-reversal invariant topological superconductor can host one Majorana cone for closed Fermi surfaces. Interestingly, there are two Majorana cones when the Fermi surfaces become open. In addition, a second-order topological superconductor with chiral Majorana states can be realized in the presence of a mixture of s±- and $id$-wave pairing. We show that chiral topological semimetals are fascinating platforms for exploring intrinsic unconventional superconductivity and topological superconductivity.