2018
DOI: 10.1103/physreva.98.013825
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Excitation and propagation of surface polaritonic rogue waves and breathers

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Cited by 26 publications
(18 citation statements)
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“…We establish that this plasmonic system generates coherent SPP amplification without the need for population inversion. These driving and signal fields have Rabi frequencies d and s , respectively, that are tightly confined to the interface by transversely evanescence coupling functions ζ d (z) and ζ s (z) 6,29 , through � m := ζ m (z)� m ; m ∈ {d, s} and we take into account the plasmonic evanescence coupling by employing field averaging technique (i.e. �ζ(z)� l � � → � l…”
Section: Brief Description Of Sspp Launching and Spp Lasing Operationmentioning
confidence: 99%
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“…We establish that this plasmonic system generates coherent SPP amplification without the need for population inversion. These driving and signal fields have Rabi frequencies d and s , respectively, that are tightly confined to the interface by transversely evanescence coupling functions ζ d (z) and ζ s (z) 6,29 , through � m := ζ m (z)� m ; m ∈ {d, s} and we take into account the plasmonic evanescence coupling by employing field averaging technique (i.e. �ζ(z)� l � � → � l…”
Section: Brief Description Of Sspp Launching and Spp Lasing Operationmentioning
confidence: 99%
“…The plasmonic field are highly dissipative for q ≫ k SPP and ω ≫ ω SPP due to Ohmic loss and atomic medium absorption. Therefore we assume a small deviation q ≈ k SPP + O(q − k SPP ) and ω = ω SPP + v SPP δω + O(δω 2 ) to this perturbation parameters 5,29 . The plasmonic mode will stably propagate within interface that its optical properties are described by macroscopic Drude-Lorentz model 28,75 .…”
mentioning
confidence: 99%
“…We also consider the seeded noise as a perturbation with amplitude u N = 0.08u 0 and modulation frequency ν mod as ∆u N = u N cos[2πν mod t] that introduces a small modification. Here the phase dynamics are then obtained by numerically solving the nonlinear Schrödinger equation [15,17,26] for u(x = 0, t) = U 0 (x = 0, t) + ∆u N . The Fourier spectrum of these NSPPs would also yield plasmonic frequency combs as we depict in Figs.…”
Section: A Universal Frequency Combs Generationmentioning
confidence: 99%
“…Besides, their application remains unexplored.Previous investigations show that the interface between a dielectric and a metallic layer is highly nonlinear and SPWs hence can propagate as various types of nonlinear optical waves such as soliton, rogue waves and breathers [41,42]. On the other hand, many proposals indicate that the optical properties of the linear and nonlinear SPWs can be controlled [27,28,41], and stable propagation of surface polaritonic solitons, rogue waves and breathers can be achieved by employing a hybrid plasmonic waveguide comprising a negative index-metamaterial(NIMM) layer and a thin atomic medium layer [42].Excited bright surface-polaritonic breathers have applications to plasmonic-phase modulation [43] and polaritonic frequency-comb generation [44,45]. Therefore, natural questions that appear are whether the darksurface polaritonic rogue waves can be excited by stable propagation and nonlinear interaction of multimode SPWs, whether they are controllable and what would be the application of these nonlinear polaritonic dark rogue waves.…”
mentioning
confidence: 99%
“…Previous investigations show that the interface between a dielectric and a metallic layer is highly nonlinear and SPWs hence can propagate as various types of nonlinear optical waves such as soliton, rogue waves and breathers [41,42]. On the other hand, many proposals indicate that the optical properties of the linear and nonlinear SPWs can be controlled [27,28,41], and stable propagation of surface polaritonic solitons, rogue waves and breathers can be achieved by employing a hybrid plasmonic waveguide comprising a negative index-metamaterial(NIMM) layer and a thin atomic medium layer [42].…”
mentioning
confidence: 99%