| Literature DB >> 27558142 |
Maryam Salehi1, Hassan Shapourian2, Nikesh Koirala3, Matthew J Brahlek3, Jisoo Moon3, Seongshik Oh3.
Abstract
In a topological insulator (TI), if its spin-orbit coupling (SOC) strength is gradually reduced, the TI eventually transforms into a trivial insulator beyond a critical point of SOC, at which point the bulk gap closes: this is the standard description of the topological phase transition (TPT). However, this description of TPT, driven solely by the SOC (or something equivalent) and followed by closing and reopening of the bulk band gap, is valid only for infinite-size samples, and little is known how TPT occurs for finite-size samples. Here, using both systematic transport measurements on interface-engineered (Bi1-xInx)2Se3 thin films and theoretical simulations (with animations in the Supporting Information), we show that description of TPT in finite-size samples needs to be substantially modified from the conventional picture of TPT due to surface-state hybridization and bulk confinement effects. We also show that the finite-size TPT is composed of two separate transitions, topological-normal transition (TNT) and metal-insulator transition (MIT), by providing a detailed phase diagram in the two-dimensional phase space of sample size and SOC strength.Entities:
Keywords: Topological insulator; metal to insulator transition; molecular beam epitaxy; thin films; topological phase transition
Year: 2016 PMID: 27558142 DOI: 10.1021/acs.nanolett.6b02044
Source DB: PubMed Journal: Nano Lett ISSN: 1530-6984 Impact factor: 11.189