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Annalen der Physik

Steady states and non‐Hermitian dynamics

Peter Schmitteckert

Published May 3, 2012• 2 citations
Publisher
DOI
10.1002/andp.201200725

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We study the dynamical properties in a non-Hermitian Bose-Hubbard dimer and show that the steady state consists mostly of the eigenstate whose eigenvalue has the largest imaginary part. A sharp phase transition occurs in the steady state and the phase transition occurs for a finite particle number, not for infinite ones, in contrast to the Hermitian system. We also investigate the quantum Fisher information and entanglement in two different phases. The results show that the steady state in the Josephson oscillation regime is fully N -particle entangled and the corresponding parameter sensitivity approaches the Heisenberg limit. In the self-trapping regime, the parameter sensitivity just scales as the shot-noise limit. Moreover, quantum Fisher information of the steady state is robust to the initial state, which indicates that the non-Hermitian dynamics takes more advantage than the Hermitian one for quantum metrology.
While the band theory of non-Hermitian Hamiltonians and the dynamics they generate have received considerable recent interest, the quantum steady states of such models remain largely unexplored. Here, the authors systematically characterize such states for fermions and bosons using an open quantum system approach. Surprisingly, these steady states exhibit features that cannot be extracted readily from the non-Hermitian Hamiltonian. This includes a macroscopic length scale which characterizes the steady-state occupation but differs from the localization length of the eigenvectors.