Abstract
Motivated by the recent prediction of anisotropy in piezoresistance of ballistic graphene along longitudinal and transverse directions, we investigate the angular gauge factor of graphene in the ballistic and diffusive regimes using highly efficient quantum transport models. It is shown that the angular guage factor in both ballistic and diffusive graphene between $0^{\circ}$ to $90^{\circ}$ bears a sinusoidal relation with a periodicity of $\pi$ due to the reduction of six-fold symmetry into a two-fold symmetry as a result of applied strain. The angular gauge factor is zero at critical angles $20^{\circ}$ and $56^{\circ}$ in ballistic and diffusive regimes respectively. Based on these findings, we propose a graphene based ballistic nano-sensor which can be used as a reference piezoresistor in a Wheatstone bridge read-out technique. The reference sensors proposed here are unsusceptible to inherent residual strain present in strain sensors and unwanted strain generated by the vapours in explosives detection. The theoretical models developed in this paper can be applied to explore similar applications in other 2D-Dirac materials. The proposals made here potentially pave the way for implementation of NEMS strain sensors based on the principle of ballistic transport, which will eventually replace MEMS piezoresistance sensors with a decrease in feature size. The presence of strain insenstive ``critical angle'' in graphene may be useful in flexible wearable electronics also.
Highlights
The development of microelectromechanical/nanoelectromechanical systems (MEMS/NEMS) has brought significant changes in every aspect of human life
The presence of strain-insensitive “critical angle” in graphene may be useful in flexible wearable electronics
It was shown that the angular gauge factor in both ballistic and diffusive graphene between 0◦ to 90◦ bears a sinusoidal relation with a periodicity of π due to the reduction of sixfold symmetry into twofold symmetry as a result of applied strain
Summary
The development of microelectromechanical/nanoelectromechanical systems (MEMS/NEMS) has brought significant changes in every aspect of human life. A single-atom-thick material, possesses extraordinary electromechanical properties such as high elasticity (≈20%) [20,21], Young’s modulus (≈1 TPa) [22], mobility [23], and mean-free path (in submicron range) [23,24,25] Due to these properties, it is considered a promising material for next-generation microelectromechanical/nanoelectromechanical systems. That the AGF in ballistic and diffusive graphene is a sinusoidal function of the transport direction with a periodicity of π due to the reduction of sixfold symmetry into twofold symmetry on the application of a uniaxial strain. We develop the mathematical model to calculate the AGF of graphene across different transport regimes, explain the underlying physics for the predicted results, and discuss the applications and future scopes. The detailed derivation of mathematical expressions is given in the Appendix
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