  We investigate the effect of a quench from a one-dimensional gas with strong
and repulsive local interactions to a strongly attractive one, known as the
super-Tonks-Girardeau effect. By incorporating both an optical lattice and
non-local interactions (specifically nearest-neighbor), we discover a
previously unexplored phenomenon: the disruption of the state during the
quench, but within a specific range of interactions. Our study employs the
extended Bose-Hubbard model across various system sizes, starting with
analytical results for two atoms and progressing to few-body systems using
exact diagonalization, DMRG and TDVP methods. Finally, we use a numerical
implementation of the local density approximation for a macroscopic number of
atoms. Consistently, our findings unveil a region where the initially
self-bound structure expands due to the super-Tonks-Girardeau quench. The fast
evaporation provides a tool to characterize the phase diagram in state-of-art
experiments exploring the physics of the extended Bose-Hubbard model.
