Elsevier

Solid State Communications

Volume 270, February 2018, Pages 82-86
Solid State Communications

Communication
The mechanical design of hybrid graphene/boron nitride nanotransistors: Geometry and interface effects

https://doi.org/10.1016/j.ssc.2017.12.001Get rights and content

Highlights

  • Three likely types (hexagonal, octagonal and decagonal) were found for the interface of sheet after relaxation.

  • Considering both mechanical and electrical performances, Csingle bondB bonds at the interface results in a more promising results.

  • In some configurations, the mechanical rupture began from BN sheets.

  • Graphene sheets started to rupture due to the instability of the octagonal and decagonal shape of the interface.

  • Nitrogen atoms are better choice for bonding to carbon at the interface of the hybrid.

Abstract

From electronic point of view, graphene resembles a metal or semi-metal and boron nitride is a dielectric material (band gap = 5.9 eV). Hybridization of these two materials opens band gap of the graphene which has expansive applications in field-effect graphene transistors. In this paper, the effect of the interface structure on the mechanical properties of a hybrid graphene/boron nitride was studied. Young's modulus, fracture strain and tensile strength of the models were simulated. Three likely types (hexagonal, octagonal and decagonal) were found for the interface of hybrid sheet after relaxation. Although Csingle bondB bonds at the interface were indicated to result in more promising electrical properties, nitrogen atoms are better choice for bonding to carbon for mechanical applications.

Introduction

Graphene has no band gap and it is considered semiconductor [1], while boron nitride is a dielectric material (band gap = 5.9 eV) [2]. Hybridization of these materials opens band gap of the graphene. Based on the literature, the value for the band gap energy is related to the concentration of boron nitride in the hybrid and this variable band gap helps the hybrid adjust its properties [3].

Because of broad applications of thin films mechanical, thermal, optical and vibration properties are the most interesting, among others. Sadeghzadeh [4], [5], [6] investigated the effects of geometry, the strain rate and temperature on the mechanical and thermal properties of single- and multilayer graphene used for designing diodes and transistors. The effects of temperature and grain size on the mechanical properties of polycrystalline boron nitride in the presence of crack were also checked [7]. Mortazavi and Rémond [8] showed that Young's modulus of boron nitride nanosheets varies between 800 and 850 GPa for the different chirality directions.

There exist two important challenges in the production of graphene-based field-effect transistors (GFETs) [9], [10]. The first is related to on/off switching of such devices which is managed by putting an insulator as a dielectric in the transistors. The other challenge is associated to the interface area between graphene and the dielectric material [11]. Since boron nitride structure is very similar to that of graphene and hence, bonding between these two materials is easier than other combinations, boron nitride may be the best choice as a dielectric material in such devices [12].

Recent experimental and theoretical studies focused on the thermal, elastic, electronic and thermoelectric properties of the graphene/h-BN interface [13], [14], [15]. Despite all the previous works, there has not been enough study on the simulation of graphene/BN hybrids and their linking, interfaces other than the simulation performed by Ding et al. based on the density functional theory (DFT) [16]. They studied mechanical properties of graphene/BN hybrid in the presence of vacancies in the zigzag and armchair linking interfaces. Their results showed that the formation energy of the defective graphene/BN interface increased with increasing inflection angles. However, Young's modulus for all graphene/BN systems studied decreased with an increase in inflection angles. The intrinsic strength of the hybrid graphene/BN sheets was shown to be affected by the inflection angles, the type of interface connection, and the type of defects. They calculated Young's modulus, fracture strength and fracture strain of graphene/BN to be 744 GPa, 95 GPa and 0.17, respectively [17].

In the present study, mechanical properties of graphene/BN hybrid were studied via the molecular dynamics simulation. At first, mechanical properties of pure graphene and pure boron nitride were explored. Then, by bonding graphene and boron nitride in a way that boron nitride sheet was placed between two single-layer graphene sheets, mechanical properties of the hybrid were investigated. The outcome of the present research may be significant for understanding the mechanism of graphene-BN interconnection and the development of corresponding devices such as graphene-based diodes and transistors.

Section snippets

Theory and model

Simulation was performed by Large-scale Atomic/Molecular Massively Parallel Simulator (LAMMPS) [18]. The interaction between carbon atoms in graphene was described by Tersoff potential parameters reported by Lindsay et al. [19]. The interaction between nitrogen and boron was described by Tersoff potential parameters developed by Matsunga et al. [20].

All simulations were conducted in the equilibrium state (EMD), and began at the constant temperature and constant pressure (NPT ensemble) with

Mechanical properties of graphene/BN hybrid

In the simulation of the hybrid, two general conditions can be considered. The first is a configuration in which the edge-to-edge linking of the graphene and boron nitride repeats successively and in the second one, the BN sheet can be placed between two graphene ribbons. The latest case was depicted in Fig. 1.

Various interface arrangements

Bonding energies of Csingle bondC, Nsingle bondB, Csingle bondN and Csingle bondB are 607, 389, 770 and 448 kcal/mol, respectively [24]. The arrangements depicted in Fig. 2 are the most probable ones out of 36 possible arrangements

Conclusion

Hybridization of graphene and BN has intrigued many researchers, as this combination converts graphene from a semiconductor with band-gap zero to a semiconductor with band-gap non-zero can have many applications in graphene-based transistors. It was observed that if carbon atoms bond to nitrogen atoms at the interface, higher mechanical properties would be obtained. On the other hand, if carbon bonds to boron at the interface, the band gap energy would be increased and semiconducting behavior

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