Effects of a Uniform Magnetic Field on Twisted Graphene Nanoribbons

Abstract

In the present work, the relativistic quantum motion of massless fermions in a helicoidal graphene nanoribbon under the influence of a uniform magnetic field is investigated. Considering a uniform magnetic field (B) aligned along the axis of helicoid, this problem is explored in the context of Dirac equation in a curved space-time. As this system does not support exact solutions due to considered background, the bound-state solutions and local density of states (LDOS) are obtained numerically by means of the Numerov method. The combined effects of width of the nanoribbon (D), length of ribbon (L), twist parameter (𝝎), and B on the equations of motion and LDOS are analyzed and discussed. It is verified that the presence of B produces a constant minimum value of local density of state on the axis of helicoid, which is possible only for values large enough of 𝝎, in contrast to the case for B = 0 already studied in the literature.

Charged scalar bosons in a Bonnor–Melvin-$$\varLambda $$ universe at conical approximation

“…To accomplish this, we consider a four-vector potential, A μ , in curved space associated with this external field. This potential is defined as A μ = e μ ā A ā , where A ā represents the fourvector potential in flat space-time [39][40][41]. In this case, we consider A ā in the form…”