journal article·2013-04

Monolayer graphene/hexagonal boron nitride heterostructure

Nikhil Jain, Tanesh Bansal, Christopher A. Durcan, Yang Xu, Bin Yu

Carbon· Volume 54
Publisher page

Abstract

Abstract A buried metal-gate field-effect transistor (FET) using a stacked hexagonal boron nitride ( h -BN) and chemically vapor deposited (CVD) graphene heterostructure is demonstrated. A thin h -BN multilayer serves as both gate dielectric and supporting layer for the monolayer graphene channel. It is observed that electrical stressing could significantly improve graphene conduction, similar to the effect reported in the graphene/SiO 2 system. In the graphene/ h -BN/TiN FET structure, p-type doping behavior in graphene is observed, possibly attributed to spontaneous doping due to the work function difference between the graphene channel and the metal gate electrode. At a high-level of stress, graphene exhibits n-type doping behavior due to charge transfer across the thin h -BN multilayer. The dielectric strength and tunneling behavior of h -BN are investigated, showing the robust nature of the layer-structured insulator.
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Research context

OpenAlex topics: Graphene research and applications · 2D Materials and Applications · Thermal properties of materials

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (23)

Show source-provided references
1. Two-dimensional gas of massless Dirac fermions in graphene10.1038/nature04233 ↗
2. A graphene field-effect device10.1109/LED.2007.891668 ↗
3. Superior thermal conductivity of single-layer graphene10.1021/nl0731872 ↗
4. Electromechanical robustness of monolayer graphene with extreme bending10.1063/1.3519982 ↗
5. 100-GHz Transistors from Wafer-Scale Epitaxial Graphene10.1126/science.1184289 ↗
6. Yu T, Kim E, Jain N, Xu Y, Geer R, Yu B. Carbon-based interconnect: performance, scaling and reliability of 3D stacked multilayer graphene system. In: IEEE international electron devices meeting; 2011, pp. 751–4.10.1109/IEDM.2011.6131508 ↗
7. Three-dimensional flexible and conductive interconnected graphene networks grown by chemical vapour deposition10.1038/nmat3001 ↗
8. Han S-J, Valdes-Garcia A, Bol AA, Franklin AD, Farmer D, Kratschmer E, et al. Graphene technology with inverted-T gate and RF passives on 200 mm platform. In: IEEE international electron devices meeting; 2011, pp. 221-4.10.1109/IEDM.2011.6131473 ↗
9. Intrinsic and extrinsic performance limits of graphene devices on SiO210.1038/nnano.2008.58 ↗
10. Ultrahigh electron mobility in suspended graphene10.1016/j.ssc.2008.02.024 ↗
11. Scanning tunnelling microscopy and spectroscopy of ultra-flat graphene on hexagonal boron nitride10.1038/nmat2968 ↗
12. Boron nitride substrates for high-quality graphene electronics10.1038/nnano.2010.172 ↗
13. Bilayer Graphene System: Current-Induced Reliability Limit10.1109/LED.2010.2058994 ↗
14. Graphene-based interconnects on hexagonal boron nitride substrate10.1109/LED.2012.2196669 ↗
15. Heat capacity and thermal conductivity of hexagonal pyrolytic boron nitride10.1103/PhysRevB.13.4607 ↗
16. Thermally limited current carrying ability of graphene nanoribbons10.1103/PhysRevLett.106.256801 ↗
17. Electrostatic doping of graphene through ultrathin hexagonal boron nitride films10.1021/nl202131q ↗
18. Doping graphene with metal contacts10.1103/PhysRevLett.101.026803 ↗
19. Electron tunneling through atomically flat and ultrathin hexagonal boron nitride10.1063/1.3662043 ↗
20. Magnetic states and optical properties of single-layer carbon-doped hexagonal boron nitride10.1063/1.4730392 ↗
21. Stability and electronic structure of potassium-intercalated hexagonal boron nitride from density functional calculations10.1103/PhysRevB.81.233401 ↗
22. Intercalation of hexagonal boron nitride by strong oxidizers and evidence for the metallic nature of the products10.1006/jssc.1999.8176 ↗
23. Logic inverter implemented with CVD-assembled graphene FET on hexagonal boron nitride10.1109/TNANO.2012.2188413 ↗