Quantum lattice transport along an infinitely extended perturbation
We consider a periodic quantum graph in the form of a rectangular lattice with the $δ$-coupling of strength $γ$ in the vertices perturbed by changing the latter at an infinite straight array of vertices to a $\widetildeγ\neγ$. We analyze the band spectrum of the system and show that it remains preserved as a set provided $\widetildeγ>γ>0$ while for all the other combinations additional band appear in some or all gaps of the unperturbed system. We also prove that for a randomly chosen positive energy, the probability of existence of a state exponentially localized in the vicinity of the perturbation equals $\frac12$.