In the resonant Bose-Hubbard model, strong-interaction effective Hamiltonians for n-boson slinky motion are generalized SSH chains with non-trivial Zak phases whose edge states appear as n-boson bound states detectable by quench dynamics.
Topological insulators with inversion symmetry
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Topological quantum slinky motion in resonant extended Bose-Hubbard model
In the resonant Bose-Hubbard model, strong-interaction effective Hamiltonians for n-boson slinky motion are generalized SSH chains with non-trivial Zak phases whose edge states appear as n-boson bound states detectable by quench dynamics.