Nonlinear propagation of incoherent waves in single-mode fibers: from wave turbulence theory to experiments

Author(s):  
Stephane Randoux ◽  
Pierre Suret ◽  
Antonio Picozzi
2011 ◽  
Author(s):  
Jing Liu ◽  
Anting Wang ◽  
Lixin Xu ◽  
Hai Ming

Mathematics ◽  
2019 ◽  
Vol 7 (11) ◽  
pp. 1067
Author(s):  
Denys Dutykh

This article is devoted to Feller’s diffusion equation, which arises naturally in probability and physics (e.g., wave turbulence theory). If discretized naively, this equation may represent serious numerical difficulties since the diffusion coefficient is practically unbounded and most of its solutions are weakly divergent at the origin. In order to overcome these difficulties, we reformulate this equation using some ideas from the Lagrangian fluid mechanics. This allows us to obtain a numerical scheme with a rather generous stability condition. Finally, the algorithm admits an elegant implementation, and the corresponding Matlab code is provided with this article under an open source license.


1974 ◽  
Vol 29 (9) ◽  
pp. 1258-1266
Author(s):  
W. Wonneberger

The problem of the natural spectral line width ⊿ω oi individual waves of a coupled many wave system in non-thermal equilibrium is discussed within the Fokker Planck approach to fluctuation phenomena. Edwards' method in turbulence theory is reinterpreted to relate ⊿ω via a modified energy balance equation to the spectrum of the mean wave intensities. This equation is solved for a model of the non-resonant feedback laser. ⊿ω is found to consist of two contributions: The first one is associated with the usual internal noise of a "free" Gaussian wave due to spontaneous emissions. Its contribution to the line width is twice that of a single mode laser far above threshold as found earlier by Brunner and Paul. The second and new contribution stems from the wave-wave coupling. It is similar to half the effective intensity fluctuation line width of the single mode laser and thus dominates above threshold.


2011 ◽  
Vol 375 (35) ◽  
pp. 3149-3155 ◽  
Author(s):  
Bertrand Kibler ◽  
Kamal Hammani ◽  
Claire Michel ◽  
Christophe Finot ◽  
Antonio Picozzi

Entropy ◽  
2019 ◽  
Vol 21 (9) ◽  
pp. 823
Author(s):  
Sergey Nazarenko ◽  
Avy Soffer ◽  
Minh-Binh Tran

We derive new kinetic and a porous medium equations from the nonlinear Schrödinger equation with random potentials. The kinetic equation has a very similar form compared to the four-wave turbulence kinetic equation in the wave turbulence theory. Moreover, we construct a class of self-similar solutions for the porous medium equation. These solutions spread with time, and this fact answers the “weak turbulence” question for the nonlinear Schrödinger equation with random potentials. We also derive Ohm’s law for the porous medium equation.


2007 ◽  
Vol 73 (5) ◽  
pp. 723-730 ◽  
Author(s):  
FOUAD SAHRAOUI ◽  
SÉBASTIEN GALTIER ◽  
GÉRARD BELMONT

AbstractHall magnetohydrodynamics (HMHD) is a mono-fluid approximation extending the validity domain of the ordinary MHD system to spatial scales down to a fraction of the ion skin depth or frequencies comparable to the ion gyrofrequency. In the paper by Galtier (2006 J. Plasma Physics), an incompressible limit of the HMHD system is used for developing a wave turbulence theory. Nevertheless, the possibility and the consequences of such an approximation are different in HMHD and in MHD. Here, we analyse these differences by investigating the properties of the HMHD equations in the incompressible limit: the existence of linear modes, their dispersion relations and polarizations. We discuss the possibility of replacing the fluid closure equation of a complete HMHD system by an incompressibility hypothesis and determine the validity range.


2021 ◽  
Vol 10 (1) ◽  
Author(s):  
Tian Dong ◽  
Jiujiu Liang ◽  
Sarah Camayd-Muñoz ◽  
Yueyang Liu ◽  
Haoning Tang ◽  
...  

AbstractLight travels in a zero-index medium without accumulating a spatial phase, resulting in perfect spatial coherence. Such coherence brings several potential applications, including arbitrarily shaped waveguides, phase-mismatch-free nonlinear propagation, large-area single-mode lasers, and extended superradiance. A promising platform to achieve these applications is an integrated Dirac-cone material that features an impedance-matched zero index. Although an integrated Dirac-cone material eliminates ohmic losses via its purely dielectric structure, it still entails out-of-plane radiation loss, limiting its applications to a small scale. We design an ultra-low-loss integrated Dirac cone material by achieving destructive interference above and below the material. The material consists of a square array of low-aspect-ratio silicon pillars embedded in silicon dioxide, featuring easy fabrication using a standard planar process. This design paves the way for leveraging the perfect spatial coherence of large-area zero-index materials in linear, nonlinear, and quantum optics.


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