To assist the design of novel, highly efficient molecular junctions, a deep
understanding of the precise charge transport mechanisms through these devices
is of prime importance. In the present contribution, we describe a procedure to
investigate spatially-resolved electron transport through a nanojunction from
first principles, at the example of a nitro-substituted oligo-(phenylene
ethynylene) covalently bound to graphene nanoribbon leads. Recently, we
demonstrated that the conductivity of this single-molecule-graphene-nanoribbon
junction can be switched quantitatively and reversibly upon application of a
static electric field in a top gate position, in the spirit of a traditional
field effect transistor [J. Phys. Chem. C, 2016, 120, 28808-28819]. The
propensity of the central oligomer unit to align with the external field was
found to induce a damped rotational motion and to cause an interruption of the
conjugated π-system, thereby drastically reducing the conductance through
the nanojunction. In the current work, we use the driven Liouville-von-Neumann
(DLvN) approach for time-dependent electronic transport calculations to
simulate the electronic current dynamics under time-dependent potential biases
for the two logical states of the nanojunction. Our quantum dynamical
simulations rely on a novel localization procedure using an orthonormal set of
molecular orbitals obtained from a standard density functional theory
calculation to generate a localized representation for the different parts of
the molecular junction. The transparent DLvN formalism allows us to directly
access the density matrix and to reconstruct the time-dependent electronic
current density, unraveling unique mechanistic details of the electron
transport