Soliton hopping in a photonic dimer arises via a subcritical Hopf bifurcation from a stable soliton branch, while in a trimer it arises supercritically from an already unstable branch, leading to different pump power thresholds and observable regimes.
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Nonlinear periodic orbit solutions and their bifurcation structure at the origin of soliton hopping in coupled microresonators
Soliton hopping in a photonic dimer arises via a subcritical Hopf bifurcation from a stable soliton branch, while in a trimer it arises supercritically from an already unstable branch, leading to different pump power thresholds and observable regimes.