
nanomaterials Review Two-Dimensional Silicon Carbide: Emerging Direct Band Gap Semiconductor Sakineh Chabi * and Kushal Kadel Department of Mechanical Engineering, University of New Mexico, Albuquerque, NM 87131, USA; [email protected] * Correspondence: [email protected] Received: 8 October 2020; Accepted: 6 November 2020; Published: 9 November 2020 Abstract: As a direct wide bandgap semiconducting material, two-dimensional, 2D, silicon carbide has the potential to bring revolutionary advances into optoelectronic and electronic devices. It can overcome current limitations with silicon, bulk SiC, and gapless graphene. In addition to SiC, which is the most stable form of monolayer silicon carbide, other compositions, i.e., SixCy, are also predicted to be energetically favorable. Depending on the stoichiometry and bonding, monolayer SixCy may behave as a semiconductor, semimetal or topological insulator. With different Si/C ratios, the emerging 2D silicon carbide materials could attain novel electronic, optical, magnetic, mechanical, and chemical properties that go beyond those of graphene, silicene, and already discovered 2D semiconducting materials. This paper summarizes key findings in 2D SiC and provides insight into how changing the arrangement of silicon and carbon atoms in SiC will unlock incredible electronic, magnetic, and optical properties. It also highlights the significance of these properties for electronics, optoelectronics, magnetic, and energy devices. Finally, it will discuss potential synthesis approaches that can be used to grow 2D silicon carbide. Keywords: silicon carbide; two-dimensional materials; semiconductor; optoelectronics 1. Introduction The discovery of monolayer silicon carbide will accelerate various technological innovations in the post-Moore era. As a wide bandgap semiconducting material with high thermal capability, SiC is a leading material for high-power electronics and high- temperature applications. However, due to quantum confinement and surface effects, 2D SiC offers tremendous unprecedented properties, which are absent in bulk SiC materials [1–5]. Unlike graphene, which is a pure one atom carbon material, 2D silicon carbide is a heteroatomic material that may exist in a variety of compositions and hence structures i.e., SixCy e.g., SiC, SiC3, SiC7, among others. Further, unlike graphene which can be exfoliated from bulk graphite via mechanical exfoliation, the synthesis of single-layer SiC is one of the most challenging and tricky syntheses among 2D materials, demanding deep understanding of the atomic structure of the bulk SiC and its crystal structures. The main challenge is that bulk SiC is not a layered van der Waals material. It is a covalently bonded material with sp3 bonding between carbon and silicon along the c axis. As such, the formation of a monolayer silicon carbide requires phase transformation from sp3 to sp2. These structural challenges lead to the following fundamental questions: How will hexagonal 2D SiC be isolated from the tetrahedrally coordinated bulk SiC if the top-down approach would be adopted? Additionally, how easy would be the phase transformation from sp3 to sp2? Or at what thickness does the transformation take place? Furthermore, how stable is 2D SiC? Does it have ideal planar structure or slightly buckled form? And more importantly is 2D SiC stable in air? Or is it highly reactive? Nanomaterials 2020, 10, 2226; doi:10.3390/nano10112226 www.mdpi.com/journal/nanomaterials Nanomaterials 2020, 10, x FOR PEER REVIEW 2 of 19 Herein, we address these outstanding questions by reviewing the latest efforts and progress in the field of 2D silicon carbide, focusing on the structure, properties, and potential applications of these emerging 2D materials. This paper is organized as follows. The first section will provide a fundamental understating of the structure of 2D silicon carbide. Then, the key properties of 2D SiC will be discussed. Finally, we will outline future opportunities and challenges. Nanomaterials 2020, 10, 2226 2 of 20 2. The Structure of 2D Silicon Carbide Structurally,Herein, we address 2D SiC these is predicted outstanding to have questions a graphene-like by reviewing honeycomb the latest eff stortsructure and progressconsisting in theof alternatingfield of 2D Si silicon and C carbide, atoms. focusingIn the monolayer on the structure, SiC, the properties, carbon and and silicon potential atoms applications will bond through of these emerging hybrid 2D orbitals materials. to form This the paper SiC is sheet, organized Figure as follows.1. Various The research first section groups will providehave investigated a fundamental the stabilityunderstating of planar of the 2D structure SiC, and of all 2D these silicon studies carbide. have Then, confirmed the key that properties 2D SiC ofis 2Denergetically SiC will be stable discussed. and hasFinally, a 100% we planar will outline structure future with opportunities inherent dynamic and challenges. stability [6–8]. They found that, while there may be a competition between hybridization preferred by C in its planar form and preferred by Si,2. Thethe ground Structure state of of 2D 2D Silicon SiC is Carbidecompletely flat, as planar 2D SiC has the lowest energy [9–11]. TheStructurally, predicted 2D planarity SiC is predicted feature is to very have aimportant, graphene-like and honeycombit contributes structure significantly consisting to the of developmentalternating Si of and several C atoms. unprecedented In the monolayer properties. SiC, the In carbon fact, except and silicon graphene atoms and will hexagonal bond through boronsp2 nitride,hybrid orbitalsh-BN, most to form of the the explored SiC sheet, 2D Figure materials,1. Various do not research have stable groups planar have investigatedstructures. Instead, the stability they stabilizeof planar their 2D SiC,monolayer and all thesestructures studies viahave i.e., a confirmed mix of that/ 2D bonding SiC is energetically i.e., buckling. stable For andinstance, has a buckling100% planar values structure of 0.44 withÅ, 0.65 inherent Å and dynamic 2.3 Å have stability been reported [6–8]. They for foundsilicene, that, germanene, while there and may black be phosphorousa competition (BP), between respectivelysp2 hybridization [11–15]. In preferred the case by of C silicene, in its planar it was form even and suggestedsp3 preferred that byone Si, approachthe ground to statereducing of 2D buckling SiC is completely level is to flat,use alternate as planar atoms 2D SiC instead has the of lowest pure silicon. energy Thus, [9–11 ].given that 2D SiCThe could predicted be considered planarity as featurea heteroatomic is very form important, of silicene, and it is contributes reasonable significantlythat it has a tostable the planardevelopment structure. of several unprecedented properties. In fact, except graphene and hexagonal boron nitride,As shown h-BN, in most Figure of the1e, exploredside view 2Dof silicene, materials, as a do result not haveof mixed stable hybridization, planar structures. sp3 and Instead,sp2, the bondsthey stabilize between their adjacent monolayer atoms structures of the silicene via i.e., lattice a mix ofaresp buckled,3/sp2 bonding resulting i.e., buckling.in a layer For that instance, is not completelybuckling values flat. It of is 0.44 of note Å, 0.65 to mention Å and 2.3 that Å havelike graphite, been reported blackfor phosphorous silicene, germanene, is a van der and Waals black layeredphosphorous material. (BP), The respectively buckling [charac11–15].ter In affects the case the of properties silicene, it of was 2D even buckled suggested materials that significantly. one approach Forto reducing instance, buckling because level silicene is to use does alternate not have atoms a insteadperfect ofplanar pure silicon.structure, Thus, it givenhas a that lower 2D SiCintrinsic could electron/holebe considered mobility as a heteroatomic than graphene. form of silicene, it is reasonable that it has a stable planar structure. FigureFigure 1. SchematicsSchematics ofof crystal crystal structure structure of grapheneof graphene (a) and(a) 2Dand SiC 2D (b SiC). Reported (b). Reported buckling buckling for different for different2D materials. 2D materials. (c) Unlike (c silicene) Unlike and silicene black and phosphorous black phosphor (BP), 2Dous SiC (BP), is 100% 2D SiC planar. is 100% (c) isplanar. reproduced (c) is reproducedfrom ref [15 ].from Atomic ref [15]. Structure Atomic of 2D Structure black phosphorus of 2D black (d ).phosphorus Credit: Institute (d). Credit: for Basic Institute Science. for Atomic Basic Science.structure Atomic of silicene structure (e). Reprinted of silicene by (e permission). Reprinted from by permission Nature [16 from], Copyright Nature [16], (2015). Copyright (2015). 3 2 SuccessfulAs shown application in Figure1e, of side any view 2D ofmaterials silicene, depen as a resultds firstly of mixed on the hybridization, material’s chemicalsp and andsp , environmentalthe bonds between stability. adjacent For instance, atoms of 2D the BP-based silicene lattice devices are have buckled, yet to resulting be realized, in a layerbecause that 2D is notBP sufferscompletely from flat.a lack It of is environmental of note to mention stability that [17]. like In graphite, the case blackof silicon phosphorous carbide monolayer, is a van derthere Waals has beenlayered some material. skepticism The about buckling the characterstability of aff planarects the monolayer properties SiC of 2Ddue buckled to the high materials reactivity significantly.
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