Abstract

The electronic properties of a material depend on the spatial freedom of the electron wavefunction. A well-known example is graphite, which is a conventional gapless semiconductor, while a single layer of it, graphene, exhibits extremely high electronic conductivity. Nevertheless, graphene ribbons can have different physical properties, such as a tunable band gap, ranging from gapless to a large band gap semiconductor. The purpose of this study is to investigate the electronic structure of few-layer graphene composed of a layer of graphene nanoribbons and graphene sheet(s), where quasi-one-dimensional nanoribbons can interact with a two-dimensional sheet of graphite. Using the tight-binding model for graphite, we show how different configurations of such heterostructures can affect the electronic structure, which is different from that of their components. Our results show that systems composed of semiconducting AGNRs can not be seen as two separate systems. Namely, a local gap of ∼0.6 eV at the Dirac point for dispersive bands can be opened in a bilayer configuration composed of a layer of gapless armchair nanoribbon stacked on graphene. We demonstrate that the band steepness in these structures can be tuned, highlighting their potential for electronic applications.

Abstract

The electronic properties of a material depend on the spatial freedom of the electron wavefunction. A well-known example is graphite, which is a conventional gapless semiconductor, while a single layer of it, graphene, exhibits extremely high electronic conductivity. Nevertheless, graphene ribbons can have different physical properties, such as a tunable band gap, ranging from gapless to a large band gap semiconductor. The purpose of this study is to investigate the electronic structure of few-layer graphene composed of a layer of graphene nanoribbons and graphene sheet(s), where quasi-one-dimensional nanoribbons can interact with a two-dimensional sheet of graphite. Using the tight-binding model for graphite, we show how different configurations of such heterostructures can affect the electronic structure, which is different from that of their components. Our results show that systems composed of semiconducting AGNRs can not be seen as two separate systems. Namely, a local gap of ∼0.6 eV at the Dirac point for dispersive bands can be opened in a bilayer configuration composed of a layer of gapless armchair nanoribbon stacked on graphene. We demonstrate that the band steepness in these structures can be tuned, highlighting their potential for electronic applications.

Abstract

The electronic properties of a material depend on the spatial freedom of the electron wavefunction. A well-known example is graphite, which is a conventional gapless semiconductor, while a single layer of it, graphene, exhibits extremely high electronic conductivity. Nevertheless, graphene ribbons can have different physical properties, such as a tunable band gap, ranging from gapless to a large band gap semiconductor. The purpose of this study is to investigate the electronic structure of few-layer graphene composed of a layer of graphene nanoribbons and graphene sheet(s), where quasi-one-dimensional nanoribbons can interact with a two-dimensional sheet of graphite. Using the tight-binding model for graphite, we show how different configurations of such heterostructures can affect the electronic structure, which is different from that of their components. Our results show that systems composed of semiconducting AGNRs can not be seen as two separate systems. Namely, a local gap of ∼0.6 eV at the Dirac point for dispersive bands can be opened in a bilayer configuration composed of a layer of gapless armchair nanoribbon stacked on graphene. We demonstrate that the band steepness in these structures can be tuned, highlighting their potential for electronic applications.

Abstract

The electronic properties of a material depend on the spatial freedom of the electron wavefunction. A well-known example is graphite, which is a conventional gapless semiconductor, while a single layer of it, graphene, exhibits extremely high electronic conductivity. Nevertheless, graphene ribbons can have different physical properties, such as a tunable band gap, ranging from gapless to a large band gap semiconductor. The purpose of this study is to investigate the electronic structure of few-layer graphene composed of a layer of graphene nanoribbons and graphene sheet(s), where quasi-one-dimensional nanoribbons can interact with a two-dimensional sheet of graphite. Using the tight-binding model for graphite, we show how different configurations of such heterostructures can affect the electronic structure, which is different from that of their components. Our results show that systems composed of semiconducting AGNRs can not be seen as two separate systems. Namely, a local gap of ∼0.6 eV at the Dirac point for dispersive bands can be opened in a bilayer configuration composed of a layer of gapless armchair nanoribbon stacked on graphene. We demonstrate that the band steepness in these structures can be tuned, highlighting their potential for electronic applications.