2011/04/30 by Holger Cartarius, Nimrod Moiseyev · 1 citation
Physics and Astronomy · #Quantum Mechanics and Non-Hermitian Physics #Quantum chaos and dynamical systems #Quantum, superfluid, helium dynamics #nlin.CD #physics.atom-ph
paper · pdf · doi:10.1103/physreva.84.013419
published as Phys. Rev. A 84, 013419 (2011) · 6 pages, 3 figures, additional references and comments in the text
arxiv created 2011/06/28 · openalex publication_date 2011/07/25 · arxiv updated 2011/07/27 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
The unique time signature of the survival probability exactly at the exceptional point parameters is studied here for the hydrogen atom in strong static magnetic and electric fields. We show that indeed the survival probability S(t)=|\ensuremath⟨\ensuremathψ(0)|\ensuremathψ(t)\ensuremath⟩|2 decays exactly as |1\ensuremath-at|2e^\ensuremath-\ensuremathΓEPt/\ensuremathℏ, where \ensuremathΓEP is associated with the decay rate at the exceptional point and a is a complex constant depending solely on the initial wave packet that populates exclusively the two almost degenerate states of the non-Hermitian Hamiltonian. This may open the possibility for a first experimental detection of exceptional points in a quantum system.