  Flatbands with extremely narrow bandwidths on the order of a few
mili-electron volts can appear in twisted multilayer graphene systems for
appropriate system parameters. Here we investigate the electronic structure of
a twisted bi-bilayer graphene, or twisted double bilayer graphene, to find the
parameter space where isolated flatbands can emerge as a function of twist
angle, vertical pressure, and interlayer potential differences. We find that in
twisted bi-bilayer graphene the bandwidth is generally flatter than in twisted
bilayer graphene by roughly up to a factor of two in the same parameter space
of twist angle $\theta$ and interlayer coupling $\omega$, making it in
principle simpler to tailor narrow bandwidth flatbands. Application of vertical
pressure can enhance the first magic angle in minimal models at $\theta \sim
1.05^{\circ}$ to larger values of up to $\theta \sim 1.5^{\circ}$ when $ P \sim
2.5$~GPa, where $\theta \propto \omega/ \upsilon_{F}$. Narrow bandwidths are
expected in bi-bilayers for a continuous range of small twist angles, i.e.
without magic angles, when intrinsic bilayer gaps open by electric fields, or
due to remote hopping terms. We find that moderate vertical electric fields can
contribute in lifting the degeneracy of the low energy flatbands by enhancing
the primary gap near the Dirac point and the secondary gap with the higher
energy bands. Distinct valley Chern bands are expected near $0^{\circ}$ or
$180^{\circ}$ alignments.
