2018
DOI: 10.1103/physreva.98.023825
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Superfluidity of light in nematic liquid crystals

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Cited by 19 publications
(17 citation statements)
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“…Any such experiment would need to have fine control over losses and nonlinearity strength in order to keep within the wave turbulence regime while the condensate is being built up. Liquid crystals are an attractive optical medium in this respect due to several inherently tunable parameters [88] that would assist in achieving conditions relevant to wave turbulence studies. Equation (3b) is well posed for spatially infinite domains in which the support of ρ(x) = |ψ (x)| 2 is compact, but if one seeks an equilibrium with spatially constant V and ρ the only solution is the trivial null solution (an empty domain).…”
Section: B Outlook For Wave Turbulence In Schrödinger-helmholtz Systemsmentioning
confidence: 99%
“…Any such experiment would need to have fine control over losses and nonlinearity strength in order to keep within the wave turbulence regime while the condensate is being built up. Liquid crystals are an attractive optical medium in this respect due to several inherently tunable parameters [88] that would assist in achieving conditions relevant to wave turbulence studies. Equation (3b) is well posed for spatially infinite domains in which the support of ρ(x) = |ψ (x)| 2 is compact, but if one seeks an equilibrium with spatially constant V and ρ the only solution is the trivial null solution (an empty domain).…”
Section: B Outlook For Wave Turbulence In Schrödinger-helmholtz Systemsmentioning
confidence: 99%
“…where σ is the nonlocal interaction length scale (σ ∼ d/2, with d corresponding to the diameter of the medium [10]), µ and ζ are the thermo-optical and linear absorption coefficients, respectively, and κ is the thermal conductivity. For nematic liquid crystals [8,9,19] we have that…”
Section: A the Schrödinger-newton Equations In Optical Systemsmentioning
confidence: 99%
“…Light propagating in nonlinear and nonlocal systems, under the paraxial approximation, is described by a Schrödinger-Newton system, which consists in a Schrödinger equation coupled with a Newtonian-like potential (or, more generally, a Poisson potential), where the former is responsible for describing the evolution of the envelope of the beam through the medium, and the last one for describing the distribution of the refractive index, and examples of materials where this model is used are nematic liquid crystals [8,9,12], thermo-optical materials [10,11] and quantum gases [13,14]. Indeed, the Schrödinger-Newton model is capable of describing a much wider set of systems, ranging from boson stars [10] to dark matter [11] and superfluidity [9,15], to name a few, and due to the similarities between these mathematical descriptions, this system has been proposed and used for implementing optical analogues [9][10][11]15], where systems that are hard or even impossible to study are emulated in the laboratory under controlled conditions. Over the years, many numerical models have been developed and improved to simulate this class of systems and in the last years, at our research group, we have developed a set of high-performance solvers based on GPGPU supercomputing to numerically study this class of systems, and successfully applied them in the study of superfluidity in nematic liquid crystals [9] and persistent currents in atomic gases [16].…”
Section: Introductionmentioning
confidence: 99%
“…In this work, we make use of advanced highperformance computing tools previously developed at our research group in the context of nonlinear optics [29][30][31], to detect and to explore how NMC curvature-matter models of gravity give rise to stationary large scale distributions of mass. In particular, we focus on a particular non-minimal coupled curvature-matter gravity model, where functions f 1 (R) and f 2 (R) are expanded up to the second and first order in the curvature R, respectively, and assume that matter at the relevant scales behaves as a fluid.…”
Section: Introductionmentioning
confidence: 99%