Carbon
nanotubes (CNTs) and graphene nanoribbons (GNRs) are lower-dimensional
derivatives of graphene. Similar to graphene, they exhibit high charge
mobilities; however, in contrast to graphene, they are semiconducting
and thus are suitable for electronics, optics, solar energy devices,
and other applications. Charge carrier mobilities, energies, and lifetimes
are governed by scattering with phonons, and we demonstrate, using
ab initio nonadiabatic molecular dynamics, that charge–phonon
scattering is much stronger in GNRs. Focusing on a GNR and a CNT of
similar size and electronic properties, we show that the difference
arises because of the significantly higher stiffness of the CNT. The
GNR undergoes large-scale undulating motions at ambient conditions.
Such thermal geometry distortions localize wave functions, accelerate
both elastic and inelastic charge–phonon scattering, and increase
the rates of energy and carrier losses. Even though, formally, both
CNTs and GNRs are quantum confined derivatives of graphene, charge–phonon
scattering differs significantly between them. Showing good agreement
with time-resolved photoconductivity and photoluminescence measurements,
the study demonstrates that GNRs are quite similar to molecules, such
as conjugated polymers, while CNTs exhibit extended features attributed
to bulk materials. The state-of-the-art simulations alter the traditional
view of graphene nanostructures and demonstrate that the performance
can be tuned not only by size and composition but also by stiffness
and response to thermal excitation.