Abstract
A simple model based on the divide and conquer rule and tight-binding (TB) approximation is employed for studying the role of finite size effect on the electronic properties of elongated graphene nanoribbon (GNR) heterojunctions. In our model, the GNR heterojunction is divided into three parts: a left (L) part, middle (M) part, and right (R) part. The left part is a GNR of width WL, the middle part is a GNR of width WM, and the right part is a GNR of width WR. We assume that the left and right parts of the GNR heterojunction interact with the middle part only. Under this approximation, the Hamiltonian of the system can be expressed as a block tridiagonal matrix. The matrix elements of the tridiagonal matrix are computed using real space nearest neighbor orthogonal TB approximation. The electronic structure of the GNR heterojunction is analyzed by computing the density of states. We demonstrate that for heterojunctions for which WL = WR, the band gap of the system can be tuned continuously by varying the length of the middle part, thus providing a new approach to band gap engineering in GNRs. Our TB results were compared with calculations employing divide and conquer rule in combination with density functional theory (DFT) and were found to agree nicely.
Highlights
Graphene is a two-dimensional (2D) allotrope of carbon with excellent electronic and mechanical properties, making it suitable for multiple applications in nanoscale electronics and nanophotonics.[1,2] A major deficiency in graphene’s properties is the absence of a band gap rendering it impossible for use in switching circuits.[3]
Our choice of material selection is reasonable since our goal is to study band gap engineering in graphene nanoribbon (GNR) heterojunctions
Since our goal is to study the properties of finite elongated GNR heterojunctions, we will start by using our TB formalism to study the role of finite size on the electronic properties of the 7-AGNR and the 11-AGNR
Summary
Graphene is a two-dimensional (2D) allotrope of carbon with excellent electronic and mechanical properties, making it suitable for multiple applications in nanoscale electronics and nanophotonics.[1,2] A major deficiency in graphene’s properties is the absence of a band gap rendering it impossible for use in switching circuits.[3]. Other factors such as finite size effect,[16,17] edge effect,[18,19,20,21,22,23] and the presence of strain[24,25,26,27] could be used to effectively tune the electronic properties GNRs
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