Bound states remain stable when their energy lies inside the reservoir band gap, and weak interactions make their lifetime finite but increasable by stronger system-reservoir coupling.
This yields the relations λ2 1 Ω1 = X k h2 k ωk , λ1(B1 +B †
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Exploring bosonic bound states with parallel reaction coordinates
Bound states remain stable when their energy lies inside the reservoir band gap, and weak interactions make their lifetime finite but increasable by stronger system-reservoir coupling.