“…The experimental discovery of the first Weyl semimetal in TaAs 1 gave impetus to the study of topological gapless states in real compounds. The topological features of the phase state determine the chiral surface states: in one-dimensional systems, these are the zero energy Majorana states 2,3 (the Majorana fermions), in two-dimensional systems, they are chiral edge modes localized at the boundaries 4,5 (the Dirac fermions), in three-dimensional systems they are the Weyl nodes and topological surface states 1,6,7 (the Weyl fermions). As a rule, topological surface states of fermions exist for a certain dimension of the system.…”