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Modifying the electrical properties of graphene by reversible point-ripple formation

DOI:10.1016/j.carbon.2018.11.076 期刊:Carbon 出版年份:2018 更新时间:2025-09-09 09:28:46
摘要: Strain, ripples and wrinkles in graphene reduce the charge-carrier mobility and alter the electronic behaviour. In few-layer graphene the anisotropy between the in-plane and cross-plane resistivity is altered and a band gap can be opened up. Here we demonstrate a method to reversibly induce point ripples in electrically isolated few-layer graphene with the ability to select the number of layers used for transport measurement down to single layer. During ripple formation the in-plane and cross-plane sheet resistances increase by up to 78% and 699% respectively, confirming that microscopic corrugation changes can solely account for graphene's non-ideal charge-carrier mobility. The method can also count the number of layers in few-layer graphene and is complimentary to Raman spectroscopy and atomic force microscopy when n ≤ 4. Understanding these changes is crucial to realising practical oscillators, nano-electromechanical systems and flexible electronics with graphene.
作者: Mona M. M. Alyobi,Chris J. Barnett,Paul Rees,Richard J. Cobley
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To demonstrate a method to reversibly induce point ripples in electrically isolated few-layer graphene and measure the change in transport properties, confirming that microscopic corrugation changes can solely account for graphene's non-ideal charge-carrier mobility.

The study demonstrates that electrostatic manipulation can be used to repeatedly separate out layers of few-layer graphene, and measure the change in transport as local point ripples are formed and stretched. These increasing resistances resulting from microscopic corrugations are large enough to account for reported low charge carrier mobility in graphene. The method can be extended to study other rippling effects including mechanical properties, the formation of electron-hole puddles and the formation of a band gap.

The lateral extension of the graphene manipulation is unknown, making quantitative determinations of the locally-induced strain or loading not possible. There is some ambiguity when the layers numbers go above 4, but for n ≤ 4 the method is complimentary to Raman and AFM for counting the number of layers in graphene.

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