Self-similar Charge Transport in Gapped Graphene
arXiv:1503.03412 · doi:10.1142/S0218348X16300026
Abstract
A new type of self-similar potential is used to study a multibarrier system made of graphene. Such potential is based on the traditional middle third Cantor set rule combined with a scaling of the barriers height. The resulting transmission coefficient for charge carriers, obtained using the quantum relativistic Dirac equation, shows a surprising self-similar structure. The same potential does not lead to a self-similar transmission when applied to the typical semiconductors described by the non-relativistic Schrödinger equation. The proposed system is one of the few examples in which a self-similar structure produces the same pattern in a physical property. The resulting scaling properties are investigated as a function of three parameters: the height of the main barrier, the total length of the system and the generation number of the potential. These scaling properties are first identified individually and then combined to find general analytic scaling expressions.
7 pages
References in corpus (12)
- Electric Field Effect in Atomically Thin Carbon Films
- The electronic properties of graphene
- Two Dimensional Atomic Crystals
- Chiral tunneling and the Klein paradox in graphene
- Substrate-induced band gap opening in epitaxial graphene
- Veselago Lens for Electrons: Focusing and Caustics in Graphene p-n Junctions
- Quantum Goos-Hanchen effect in graphene
- Leonardo's rule, self-similarity and wind-induced stresses in trees
- Quasi-exact solution to the Dirac equation for the hyperbolic secant potential
- Searching for confined modes in graphene channels: the variable phase method
- Tunneling of Dirac electrons through spatial regions of finite mass
- Spectral scalability as a result of geometrical self-similarity in fractal multilayers
Cited by in corpus (2)
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