2001/10/30 by Tai‐Peng Tsai, Tai-Peng Tsai, Horng-Tzer Yau +3 · 2 citations
Mathematics · Physics and Astronomy · #35Q40 #35Q55 #Advanced Mathematical Physics Problems #FOS: Physical sciences #Mathematical Physics (math-ph) #Quantum Mechanics and Non-Hermitian Physics #Spectral Theory in Mathematical Physics #math-ph #math.MP #msc:35Q40 #msc:35Q55
paper · pdf · doi:10.48550/arxiv.math-ph/0110037
v2: sec 3 changed
openalex publication_date 2001/10/30 · arxiv created 2002/01/02 · arxiv updated 2016/09/07 · openalex created_date 2025/10/24 · openalex updated_date 2026/07/28
We consider nonlinear Schrödinger equations in \R3. Assume that the linear Hamiltonians have two bound states. For certain finite codimension subset in the space of initial data, we construct solutions converging to the excited states in both non-resonant and resonant cases. In the resonant case, the linearized operators around the excited states are non-self adjoint perturbations to some linear Hamiltonians with embedded eigenvalues. Although self-adjoint perturbation turns embedded eigenvalues into resonances, this class of non-self adjoint perturbations turn an embedded eigenvalue into two eigenvalues with the distance to the continuous spectrum given to the leading order by the Fermi golden rule.