Nonlinearly PT-symmetric systems: Spontaneous symmetry breaking and transmission resonances
By Andrey Miroshnichenko, Boris A. Malomed, Yuri Kivshar. 2011
164 citations recorded by the source corpus.
We consider a class of $\mathcal{PT}$-symmetric systems which include mutually matched nonlinear loss and gain (in other words, a class of $\mathcal{PT}$-invariant Hamiltonians in which both the harmonic and anharmonic parts are non-Hermitian). For a basic system in the form of a dimer, symmetric and asymmetric eigenstates, including multistable ones, are found analytically. We demonstrate that, if coupled to a linear chain, such a nonlinear $\mathcal{PT}$-symmetric dimer generates previously unexplored types of nonlinear Fano resonances, with completely suppressed or greatly amplified transmission, as well as a regime similar to the electromagnetically induced transparency. The implementation of the systems is possible in various media admitting controllable linear and nonlinear amplification of waves.
Subfields: Atomic and Molecular Physics, and Optics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/72b414e427a60ecad6a10fef713e5ecebacc43e0
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In Atomic and Molecular Physics, and Optics
- Jianke Yang
- Dmitry A. Zezyulin
- Sergey V. Dmitriev
- Chao-Kuei Lee
- Jiahao Huang
- Vladimir V. Konotop
- A. Sukhorukov
- S. Suchkov
In Statistical and Nonlinear Physics
- Jianke Yang
- Dmitry A. Zezyulin
- Sergey V. Dmitriev
- Chao-Kuei Lee
- Jiahao Huang
- Vladimir V. Konotop
- A. Sukhorukov
- S. Suchkov
Citations in the corpus
- Nonlinear waves in PT -symmetric systems (2016, background): “Looking for stationary nonlinear modes in the form of q0,1 = A0,1e iφ0,1e−iEz, one can classify possible solutions into three groups (Chen et al., 2015; Duanmu et al., 2013; Miroshnichenko, Malomed, and Kivshar, 2011): a. Continuous families of PT -symmetric solutions.”
- Nonlinear switching and solitons in PT‐symmetric photonic systems (2015, background): “where the overdot stands for the time derivative, γ0 > 0 accounts for the linear gain and loss acting on complex variables ψA and ψB , respectively, E is a frequency shift, γ2 accounts for the PT-symmetric nonlinear loss and gain (as shown in [35], stable eigenstates are obtained with γ2 > 0, i.”