Decay of symmetry-protected quantum states
A. A. Bychek, D. N. Maksimov, A. R. Kolovsky

TL;DR
This paper investigates how quantum fluctuations cause decay of symmetry-protected states in a Bose-Hubbard chain, revealing that such states are metastable at finite interactions despite classical stability.
Contribution
It demonstrates that symmetry-protected quantum states in a Bose-Hubbard chain are metastable due to quantum fluctuations, contrasting classical predictions of stability.
Findings
Quantum fluctuations induce decay of symmetry-protected states.
Symmetry-protected states are metastable at finite interactions.
Classical stability does not guarantee quantum stability.
Abstract
We study the decay of bosonic many-body states in the three well Bose-Hubbard chain where bosons in the central well can escape into a reservoir. For vanishing inter-particle interaction this system supports a non-decaying many-body state which is the antisymmetric Bose-Einstein condensate with particles occupying only the edge wells. In the classical approach this quantum state corresponds to a symmetry protected non-decaying state which is stable even at finite interaction below a certain intensity threshold. Here we demonstrate that despite the classical counterpart is stable the antisymmetric Bose-Einstein condensate is always metastable at finite interatomic interactions due to quantum fluctuations.
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