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Nanomechanics and interfacial properties of supported and suspended graphene layers

Research output: Contribution to conference - Without ISBN/ISSN Abstractpeer-review

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Nanomechanics and interfacial properties of supported and suspended graphene layers. / Robinson, Benjamin; Kay, Nicholas; Mazzocco, Riccardo et al.
2013. Abstract from NanoteC13 Carbon Nanoscience and Nanotechnology, United Kingdom.

Research output: Contribution to conference - Without ISBN/ISSN Abstractpeer-review

Harvard

Robinson, B, Kay, N, Mazzocco, R & Kolosov, O 2013, 'Nanomechanics and interfacial properties of supported and suspended graphene layers', NanoteC13 Carbon Nanoscience and Nanotechnology, United Kingdom, 28/08/13.

APA

Robinson, B., Kay, N., Mazzocco, R., & Kolosov, O. (2013). Nanomechanics and interfacial properties of supported and suspended graphene layers. Abstract from NanoteC13 Carbon Nanoscience and Nanotechnology, United Kingdom.

Vancouver

Robinson B, Kay N, Mazzocco R, Kolosov O. Nanomechanics and interfacial properties of supported and suspended graphene layers. 2013. Abstract from NanoteC13 Carbon Nanoscience and Nanotechnology, United Kingdom.

Author

Robinson, Benjamin ; Kay, Nicholas ; Mazzocco, Riccardo et al. / Nanomechanics and interfacial properties of supported and suspended graphene layers. Abstract from NanoteC13 Carbon Nanoscience and Nanotechnology, United Kingdom.

Bibtex

@conference{aae2d7d6d94e412f82d8530426dad15f,
title = "Nanomechanics and interfacial properties of supported and suspended graphene layers",
abstract = "We report the nanoscale exploration of the structural, interfacial and nanomechanical properties of supported and suspended graphene films using dynamic scanning probe techniques operating in the regime of a few KHz to several MHz. Furthermore, we extend this approach to study the interaction of the graphene with local liquid environments. In order to study graphene nanostructures of 10 to several 100 nm dimensions which are both suspended and supported, the ability to probe both low and extreme stiffness range is required. For lower range stiffness we used force modulation microscopy (FMM), operating at 1-10 kHz and exploring stiffness k in the range of 0.1 to 10 N/m; whereas for k in range up to 10,000 N/m we used ultrasonic force microscopy (UFM). In UFM a sample is vibrated at low amplitude (5-10 {\AA}) and very high frequency (typically 2 – 100 MHz) which makes the cantilever dynamically extremely rigid. The ultrasonic oscillation is then amplitude modulated at low (few kHz) frequency and “rectified” owing to the extreme nonlinear force-vs-distance dependence of the tip-surface contact, resulting in a net “UFM” force at the modulation frequency that produces excellent material contrast to stiff nanostructures.We observe, with nanoscale resolution, surface and sub-surface features arising from the graphene-substrate and also the graphene-environment interactions. We can, for example, map local bending stiffness of suspended few layer graphene (FLG), elucidate growth processes of graphene films via carbon diffusion through metals and study the nanomechanics of normal (adhesive and elastic) and tangential (friction) forces between AFM tip and exfoliated FLG as a function of surrounding media",
author = "Benjamin Robinson and Nicholas Kay and Riccardo Mazzocco and Oleg Kolosov",
year = "2013",
language = "English",
note = "NanoteC13 Carbon Nanoscience and Nanotechnology ; Conference date: 28-08-2013",

}

RIS

TY - CONF

T1 - Nanomechanics and interfacial properties of supported and suspended graphene layers

AU - Robinson, Benjamin

AU - Kay, Nicholas

AU - Mazzocco, Riccardo

AU - Kolosov, Oleg

PY - 2013

Y1 - 2013

N2 - We report the nanoscale exploration of the structural, interfacial and nanomechanical properties of supported and suspended graphene films using dynamic scanning probe techniques operating in the regime of a few KHz to several MHz. Furthermore, we extend this approach to study the interaction of the graphene with local liquid environments. In order to study graphene nanostructures of 10 to several 100 nm dimensions which are both suspended and supported, the ability to probe both low and extreme stiffness range is required. For lower range stiffness we used force modulation microscopy (FMM), operating at 1-10 kHz and exploring stiffness k in the range of 0.1 to 10 N/m; whereas for k in range up to 10,000 N/m we used ultrasonic force microscopy (UFM). In UFM a sample is vibrated at low amplitude (5-10 Å) and very high frequency (typically 2 – 100 MHz) which makes the cantilever dynamically extremely rigid. The ultrasonic oscillation is then amplitude modulated at low (few kHz) frequency and “rectified” owing to the extreme nonlinear force-vs-distance dependence of the tip-surface contact, resulting in a net “UFM” force at the modulation frequency that produces excellent material contrast to stiff nanostructures.We observe, with nanoscale resolution, surface and sub-surface features arising from the graphene-substrate and also the graphene-environment interactions. We can, for example, map local bending stiffness of suspended few layer graphene (FLG), elucidate growth processes of graphene films via carbon diffusion through metals and study the nanomechanics of normal (adhesive and elastic) and tangential (friction) forces between AFM tip and exfoliated FLG as a function of surrounding media

AB - We report the nanoscale exploration of the structural, interfacial and nanomechanical properties of supported and suspended graphene films using dynamic scanning probe techniques operating in the regime of a few KHz to several MHz. Furthermore, we extend this approach to study the interaction of the graphene with local liquid environments. In order to study graphene nanostructures of 10 to several 100 nm dimensions which are both suspended and supported, the ability to probe both low and extreme stiffness range is required. For lower range stiffness we used force modulation microscopy (FMM), operating at 1-10 kHz and exploring stiffness k in the range of 0.1 to 10 N/m; whereas for k in range up to 10,000 N/m we used ultrasonic force microscopy (UFM). In UFM a sample is vibrated at low amplitude (5-10 Å) and very high frequency (typically 2 – 100 MHz) which makes the cantilever dynamically extremely rigid. The ultrasonic oscillation is then amplitude modulated at low (few kHz) frequency and “rectified” owing to the extreme nonlinear force-vs-distance dependence of the tip-surface contact, resulting in a net “UFM” force at the modulation frequency that produces excellent material contrast to stiff nanostructures.We observe, with nanoscale resolution, surface and sub-surface features arising from the graphene-substrate and also the graphene-environment interactions. We can, for example, map local bending stiffness of suspended few layer graphene (FLG), elucidate growth processes of graphene films via carbon diffusion through metals and study the nanomechanics of normal (adhesive and elastic) and tangential (friction) forces between AFM tip and exfoliated FLG as a function of surrounding media

M3 - Abstract

T2 - NanoteC13 Carbon Nanoscience and Nanotechnology

Y2 - 28 August 2013

ER -