Abstract

ABSTRACT Freestanding (suspended) graphene films, with high electron mobility (up to ~200,000 cm2V−1s−1), good mechanical and electronic properties, could resolve many of the current issues that are hampering the upscaling of graphene technology. Thus far, attempts at reliably fabricating suspended graphene devices comprising metal contacts, have often been hampered by difficulties in exceeding sizes of 1 µm in diameter, if using UV lithography. In this work, area of suspended graphene large enough to be utilized in microelectronic devices, have been obtained by suspending a CVD graphene film over cavities, with top contacts defined through UV lithography with both wet and dry etching. An area of up to 160 µm2 can be fabricated as backgated devices. The suspended areas exhibit rippling of the surfaces which simultaneously introduces both tensile and compressive strain on the graphene film. Finally, the variations of the Fermi level in the suspended graphene areas can be modulated by applying a potential difference between the top contacts and the backgate. Having achieved large area suspended graphene, in a manner compatible with CMOS fabrication processes, together with enabling the modulation of the Fermi level, are substantial steps forward in demonstrating the potential of suspended graphene-based electronic devices and sensors.

Highlights

  • Since its first isolation, graphene [1] has been hailed as a revolutionary material

  • Areas of suspended graphene have been obtained by transferring a CVD graphene film over cavities in either SU-8 or SiO2

  • We have studied a number of specimens and showed that large areas of up to 160 μm2 can be fabricated as functional backgated devices

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Summary

Introduction

Graphene [1] has been hailed as a revolutionary material. in order to enable large volume applications in the electronic and sensors sectors, graphene still needs to be produced as a large transferrable film [2,3,4]. This would suggest a significant degree of local variations in either the film uniformity, strain status or doping levels over the surface of each individual SusG area.

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