2019
DOI: 10.1038/s41598-019-53455-0
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Exceptional points in classical spin dynamics

Abstract: Non-conservative physical systems admit a special kind of spectral degeneracy, known as exceptional point (EP), at which eigenvalues and eigenvectors of the corresponding non-Hermitian Hamiltonian coalesce. Dynamical parametric encircling of the EP can lead to non-adiabatic evolution associated with a state flip, a sharp transition between the resonant modes. Physical consequences of the dynamical encircling of EPs in open dissipative systems have been explored in optics and photonics. Building on the recent p… Show more

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Cited by 19 publications
(16 citation statements)
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“…In (26), h is defined by the equation (19). As in the previous subsection, we expand the magnetisation vector over an orthonormal basis {A, B, M (0) }:…”
Section: B Perturbation Of Latitudinal Fixed Pointsmentioning
confidence: 99%
“…In (26), h is defined by the equation (19). As in the previous subsection, we expand the magnetisation vector over an orthonormal basis {A, B, M (0) }:…”
Section: B Perturbation Of Latitudinal Fixed Pointsmentioning
confidence: 99%
“…While initially EPs were regarded as a mathematical-physics concept, in the last decade there has been a growing interest on EPs from the experimental point of view in such areas as atomic spectra measurements [8] , microwave cavity experiments [9][10][11][12][13] , chaotic optical microcavities [14] or optomechanical systems [15] . Interestingly, exceptional points arise also in classical systems, such as coupled electric oscillators [16,17] , optical systems [18] , classical spin dynamics [19,20] , and general dissipative classical systems [21] .…”
mentioning
confidence: 99%
“…Very recently, there has been growing attention on EPs in the area of magnetism with theoretical works on spin dynamics [19,20,29] and spin-orbit systems [30] . Experimental results have been achieved in passive magnonic structures [31] or opto-magnonic systems [32] .…”
mentioning
confidence: 99%
“…Magnons, i.e., the collective excitations of magnetic systems, are bosonic quasiparticles whose number is not conserved and whose dynamics is intrinsically non-Hermitian [25][26][27][28][29][30]. Their fundamental properties, including their lifetime, can be easily tuned via external fields and drives, making them promising solid-state candidates for the exploration of non-Hermitian topological phenomena [31][32][33][34].…”
mentioning
confidence: 99%