Hostname: page-component-76fb5796d-2lccl Total loading time: 0 Render date: 2024-04-25T17:50:11.027Z Has data issue: false hasContentIssue false

Partially Hydrogenated Graphene: Semiconductor Material with a Tunable Gap and Its Non-Destructive Optical Characterization

Published online by Cambridge University Press:  07 July 2011

F. Gaspari
Affiliation:
University of Ontario Institute of Technology, Oshawa, ON, L1H 7K4, Canada
A.I. Shkrebtii
Affiliation:
University of Ontario Institute of Technology, Oshawa, ON, L1H 7K4, Canada
P. McNelles
Affiliation:
University of Ontario Institute of Technology, Oshawa, ON, L1H 7K4, Canada
J.L. Cabellos
Affiliation:
Centro de Investigaciones en Optica, Leon, Guanajuato, 37150, Mexico
B.S. Mendoza
Affiliation:
Centro de Investigaciones en Optica, Leon, Guanajuato, 37150, Mexico
Get access

Abstract

We report first principles modeling of partially hydrogenated graphene, with a variety of hydrogen induced superstructures. The dependence of the optical gap on hydrogen content and coverage is examined, to assess the best configurations suitable for optoelectronic applications. Electron and optical DFT LDA gaps in the range between 0.2 and 1.5 eV were obtained for low hydrogen coverage. For such systems, hydrogen clustering (by saturating neighbouring C dangling bonds at the opposite sides of the graphene sheet) is energetically most favourable and generally produces larger gap. More homogeneous H distribution one-side bonded to C-host atoms is, in contrast, less energetically favourable or even structurally unstable and generally produces smaller gap. In addition, ordering of hydrogen was observed at 50% of H, that offers a possibility of transforming 2D graphene to an array of 1D nanowires Calculated linear optical anisotropy and nonlinear second harmonic generation (this will be discussed in a forthcoming paper) indicate these are not only gap sensitive, but can provide an access to microscopic details of the 2D nano-sheets such as symmetry, hydrogen induced structure, degree of hydrogenation, chemical bonding and many others, all promising for device application. The approach developed can be used for graphene/ graphane single layer or bilayer, formed on top of various substrates, where experimental geometries may not provide conditions for complete hydrogenation of the 2D nano-sheet(s).

Type
Research Article
Copyright
Copyright © Materials Research Society 2011

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

[1] Novoselov, K. S., Geim, A. K., Morozov, S. V., et al. . Science 306, 666 (2004)Google Scholar
[2] Sofo, J. O., Chaudhari, A. S., and Barber, G. D., Phys. Rev. B 75, 153401 (2007)Google Scholar
[3] Shkrebtii, A. I., Cabellos, J. L., Arzate, N., Mendoza, B. S., and McNelles, P., International School of Solid State Physics Epioptics-11, Erice, Sicily, 19-25 July 2010 Google Scholar
[4] Haberer, D., Vyalikh, D. V., Taioli, S., et al. , Nano Letters 10, 3360 (2010)Google Scholar
[5] Elias, D. C., Nair, R. R., Mohiuddin, T. M. G., et al. , Science 323, 610 (2009)Google Scholar
[6] Fiori, G., Lebegue, S., Betti, A., et al. ., Phys. Rev. B, 82, 153404 (2010)Google Scholar
[9] Marsili, M. and Pulci, O., J. Phys. D: Appl. Phys. 43 374016 (2010)Google Scholar
[10] Cudazzo, P., Attaccalite, C., Tokatly, I.V., et al. . Phys. Rev. Lett. 104, 226804 (2010)Google Scholar
[11] Rosli, N.A., et al. ., PROGRESS OF PHYSICS RESEARCH IN MALAYSIA 269 (2010)Google Scholar
[12] Wang, Y., Xu, X., Lu, J., et al. , ACS Nano 4, 6146 (2010)Google Scholar
[13] Shkrebtii, A. I., et al. ., private communication.Google Scholar