The many-body localization (MBL) transition is a quantum phase
transition involving highly excited eigenstates of a disordered quantum
many-body Hamiltonian, which evolve from “extended/ergodic"
(exhibiting extensive entanglement entropies and fluctuations) to
“localized" (exhibiting area-law scaling of entanglement and
fluctuations). The MBL transition can be driven by the strength of
disorder in a given spectral range, or by the energy density at fixed
disorder – if the system possesses a many-body mobility edge. Here we
propose to explore the latter mechanism by using “quantum-quench
spectroscopy", namely via quantum quenches of variable width which
prepare the state of the system in a superposition of eigenstates of the
Hamiltonian within a controllable spectral region. Studying numerically
a chain of interacting spinless fermions in a quasi-periodic potential,
we argue that this system has a many-body mobility edge; and we show
that its existence translates into a clear dynamical transition in
the time evolution immediately following a quench in the strength of the
quasi-periodic potential, as well as a transition in the scaling properties of the
quasi-stationary state at long times. Our results suggest a practical scheme
for the experimental observation of many-body mobility edges using
cold-atom setups.