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Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators

We present a Raman mapping study of monolayer graphene G and 2D bands, after integration on silicon strip-waveguide-based micro-ring resonators (MRRs) to characterize the effects of the graphene transfer processes on its structural and optoelectronic properties. Analysis of the Raman G and 2D peak p...

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Autores principales: Hussein, Siham M., Crowe, Iain F., Clark, Nick, Milosevic, Milan, Vijayaraghavan, Aravind, Gardes, Frederic Y., Mashanovich, Goran Z., Halsall, Matthew P.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer US 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5700035/
https://www.ncbi.nlm.nih.gov/pubmed/29168000
http://dx.doi.org/10.1186/s11671-017-2374-4
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author Hussein, Siham M.
Crowe, Iain F.
Clark, Nick
Milosevic, Milan
Vijayaraghavan, Aravind
Gardes, Frederic Y.
Mashanovich, Goran Z.
Halsall, Matthew P.
author_facet Hussein, Siham M.
Crowe, Iain F.
Clark, Nick
Milosevic, Milan
Vijayaraghavan, Aravind
Gardes, Frederic Y.
Mashanovich, Goran Z.
Halsall, Matthew P.
author_sort Hussein, Siham M.
collection PubMed
description We present a Raman mapping study of monolayer graphene G and 2D bands, after integration on silicon strip-waveguide-based micro-ring resonators (MRRs) to characterize the effects of the graphene transfer processes on its structural and optoelectronic properties. Analysis of the Raman G and 2D peak positions and relative intensities reveal that the graphene is electrically intrinsic where it is suspended over the MRR but is moderately hole-doped where it sits on top of the waveguide structure. This is suggestive of Fermi level ‘pinning’ at the graphene-silicon heterogeneous interface, and we estimate that the Fermi level shifts down by approximately 0.2 eV from its intrinsic value, with a corresponding peak hole concentration of ~ 3 × 10(12) cm(−2). We attribute variations in observed G peak asymmetry to a combination of a ‘stiffening’ of the E (2g) optical phonon where the graphene is supported by the underlying MRR waveguide structure, as a result of this increased hole concentration, and a lowering of the degeneracy of the same mode as a result of localized out-of-plane ‘wrinkling’ (curvature effect), where the graphene is suspended. Examination of graphene integrated with two different MRR devices, one with radii of curvature r = 10 μm and the other with r = 20 μm, indicates that the device geometry has no measureable effect on the level of doping.
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spelling pubmed-57000352017-12-04 Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators Hussein, Siham M. Crowe, Iain F. Clark, Nick Milosevic, Milan Vijayaraghavan, Aravind Gardes, Frederic Y. Mashanovich, Goran Z. Halsall, Matthew P. Nanoscale Res Lett Nano Express We present a Raman mapping study of monolayer graphene G and 2D bands, after integration on silicon strip-waveguide-based micro-ring resonators (MRRs) to characterize the effects of the graphene transfer processes on its structural and optoelectronic properties. Analysis of the Raman G and 2D peak positions and relative intensities reveal that the graphene is electrically intrinsic where it is suspended over the MRR but is moderately hole-doped where it sits on top of the waveguide structure. This is suggestive of Fermi level ‘pinning’ at the graphene-silicon heterogeneous interface, and we estimate that the Fermi level shifts down by approximately 0.2 eV from its intrinsic value, with a corresponding peak hole concentration of ~ 3 × 10(12) cm(−2). We attribute variations in observed G peak asymmetry to a combination of a ‘stiffening’ of the E (2g) optical phonon where the graphene is supported by the underlying MRR waveguide structure, as a result of this increased hole concentration, and a lowering of the degeneracy of the same mode as a result of localized out-of-plane ‘wrinkling’ (curvature effect), where the graphene is suspended. Examination of graphene integrated with two different MRR devices, one with radii of curvature r = 10 μm and the other with r = 20 μm, indicates that the device geometry has no measureable effect on the level of doping. Springer US 2017-11-22 /pmc/articles/PMC5700035/ /pubmed/29168000 http://dx.doi.org/10.1186/s11671-017-2374-4 Text en © The Author(s). 2017 Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
spellingShingle Nano Express
Hussein, Siham M.
Crowe, Iain F.
Clark, Nick
Milosevic, Milan
Vijayaraghavan, Aravind
Gardes, Frederic Y.
Mashanovich, Goran Z.
Halsall, Matthew P.
Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators
title Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators
title_full Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators
title_fullStr Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators
title_full_unstemmed Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators
title_short Raman Mapping Analysis of Graphene-Integrated Silicon Micro-Ring Resonators
title_sort raman mapping analysis of graphene-integrated silicon micro-ring resonators
topic Nano Express
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5700035/
https://www.ncbi.nlm.nih.gov/pubmed/29168000
http://dx.doi.org/10.1186/s11671-017-2374-4
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