-symmetry breaking in a Kitaev chain with one pair of gain-loss potentials
arXiv:2103.07058 · doi:10.1103/PhysRevA.104.022218
Abstract
Parity-time () symmetric systems are classical, gain-loss systems whose dynamics are governed by non-Hermitian Hamiltonians with exceptional-point (EP) degeneracies. The eigenvalues of a -symmetric Hamiltonian change from real to complex conjugates at a critical value of gain-loss strength that is called the breaking threshold. Here, we obtain the -threshold for a one-dimensional, finite Kitaev chain -- a prototype for a p-wave superconductor -- in the presence of a single pair of gain and loss potentials as a function of the superconducting order parameter, on-site potential, and the distance between the gain and loss sites. In addition to a robust, non-local threshold, we find a rich phase diagram for the threshold that can be qualitatively understood in terms of the band-structure of the Hermitian Kitaev mo del. In particular, for an even chain with zero on-site potential, we find a re-entrant -symmetric phase bounded by second-order EP contours. Our numerical results are supplemented by analytical calculations for small system sizes.
8 pages, 6 figures
References in corpus (5)
- Visualization of Branch Points in PT-Symmetric Waveguides
- Observation of parity-time symmetry breaking in a single spin system
- PT-symmetry breaking and universal chirality in a PT-symmetric ring
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- Floquet topological properties in the Non-Hermitian long-range system with complex hopping amplitudes