Interplay of bulk and edge states in transport of two-dimensional topological insulators

We study transport in two-terminal metal/quantum spin Hall insulator/metal junctions. We show that the conductance signals originating from the bulk and the edge contributions are not additive. While for a long junction the transport is determined by the edge states contribution, for a short junction, the conductance signal is built from both bulk and edge states in the ratio, which depends on the width of the sample. Further, in the topological insulator regime the conductance for short junctions shows a nonmonotonic behavior as a function of the sample length. Surprisingly this nonmonotonic behavior of conductance can be traced to the formation of an effectively propagating solution, which is robust against scalar disorder. Our predictions should be experimentally verifiable in HgTe quantum wells and Bi2Se3 thin films.