Abstract

Graphene (G) and hexagonal Boron Nitride (h-BN) are structurally similar materials but have very different electronic and magnetic properties. Heterostructures formed by the combination of these materials are of great research interest. To assess the role played by the crystalline defects in such heterostructures is also of crucial importance owing to their novel properties. In the present work, we study the structural, electronic, and magnetic properties of the G/h-BN heterostructure and the different possible point defects of B and N atoms in it by using first-principles calculations based on the spin-polarized density functional theory (DFT) method within the van der Waals correction DFT-D2 approach. The structural analysis of these systems shows that they are stable two dimensional van der Waals heterostructure materials. Band structure calculations of these materials reveal their semimetallic nature. On the basis of density of states and partial density of states calculations, the defective systems are magnetic materials. The magnetic moment obtained in these defective systems is due to the unpaired up-spin and down-spin states in the orbitals of C, B, and N atoms created by the vacancy defects. On the other hand, the G/h-BN heterostructure has an approving condition for ferromagnetism due to the presence of flat bands in the neighborhood of the Fermi energy.

Highlights

  • The advent of the field of two dimensional (2D) crystals has grabbed the curiosity of physicists due to their properties worth inquiring.1,2 Researchers are attracted toward 2D graphene (G) and hexagonal-Boron Nitride (h-BN) materials because of their intriguing properties.3–6 The honeycomb structure of graphene is used in the fields of technological applications7,8 owing to its electronic and mechanical properties

  • B and N atoms are bound by strong covalent bonds, as in graphene, while the layers are held together by weak van der Waals forces, as in graphite.10 h-BN is isoelectronic with graphite, and its structure is similar except for the difference in the stacking of the layers

  • The unit cell of h-BN consists of one B atom and one N atom covalently bonded together

Read more

Summary

Introduction

The advent of the field of two dimensional (2D) crystals has grabbed the curiosity of physicists due to their properties worth inquiring. Researchers are attracted toward 2D graphene (G) and hexagonal-Boron Nitride (h-BN) materials because of their intriguing properties. The honeycomb structure of graphene (zero bandgap energy) is used in the fields of technological applications owing to its electronic and mechanical properties. The honeycomb structure of graphene (zero bandgap energy) is used in the fields of technological applications owing to its electronic and mechanical properties. Heterostructure (HS) materials are created by incorporation of two distinct monolayer constituents. GBN-I scitation.org/journal/adv material develops new thermal conductivity and electronic and magnetic properties compared with its constituents.. We have constructed the vdW G/h-BN heterostructure (GBN-I) material using graphene and h-BN with a considerable (1.4%) lattice mismatch, which is comparable with reported values.. To the best of our knowledge, the literature does not contain the study of structural, electronic, and magnetic properties of the 2D vdW graphene/h-BN heterostructure (GBN-I) and B and N site vacancy defects in GBN-I materials. In the present work, we investigated the structural, electronic, and magnetic properties of the G/h-BN heterostructure without defects (GBN-I), the one B atom vacancy defect in the G/h-BN heterostructure (GBNIB), the one N atom vacancy defect in the G/h-BN heterostructure (GBN-IN), nearest neighbor one B atom and one N atom vacancy defects in the G/h-BN heterostructure (GBN-NB), and the alternate zone of one B atom and one N atom vacancy defects in G/h-BN heterostructure (GBN-IBIN) materials through band structure analysis and density of states (DoS) and partial density of states (PDoS)

Methods
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call