2003
DOI: 10.1016/s0375-9601(03)00069-0
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Instability of vortex filaments in laser–matter interactions

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Cited by 12 publications
(22 citation statements)
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“…Here A is the perturbation amplitude equivalent to the height of the scratch wall, and k p is the perturbation wavenumber: k p = 2π/L μm −1 . An oscillatory shock perturbs the density interface (shear layer) transversally to the radial flow, or the flow from the central to the peripheral regions (y-direction), causing the formation of waves and their roll-up into vortex filaments of the core thickness σ ∼ 5−7μm [1][2][3][4]. As a result, a high density 1D array of vortex filaments (the separation distance between neighboring filaments Λ ≤ σ) has been generated.…”
Section: Outline Of Experimentsmentioning
confidence: 99%
See 1 more Smart Citation
“…Here A is the perturbation amplitude equivalent to the height of the scratch wall, and k p is the perturbation wavenumber: k p = 2π/L μm −1 . An oscillatory shock perturbs the density interface (shear layer) transversally to the radial flow, or the flow from the central to the peripheral regions (y-direction), causing the formation of waves and their roll-up into vortex filaments of the core thickness σ ∼ 5−7μm [1][2][3][4]. As a result, a high density 1D array of vortex filaments (the separation distance between neighboring filaments Λ ≤ σ) has been generated.…”
Section: Outline Of Experimentsmentioning
confidence: 99%
“…It is well known that nanosecond laser-matter interactions (LMI) may generate a one-dimensional (1D) array of vortex filaments on a solid surface, with the behavior that is common to string-like formations of various systems [1][2][3]. Among them is the action of torsion that generates the Hasimoto solitons [1], formation and instability of vortex rings [4], the phenomena like helicoidal instability, reconnection, and merging of filaments [2], looping of the filaments in the strain field of a point defect, spiraling and pinning [3] etc. All these phenomena are possible due to the fact that vortex filaments (in a certain stage of the LMI), behave as a viscoelastic entity.…”
Section: Introductionmentioning
confidence: 99%
“…Owing to ultrafast cooling at the end of pulse, the obtained pattern stays frozen permanently, which allows for a geometric analysis. Fukumoto and Lugomer (2003) clarified by a simple estimation of material parameters that the formation of vortex filaments was narrowly possible by a fortuitous adjustment of parameter values.…”
Section: Introductionmentioning
confidence: 99%
“…As a scenario of formation of vortex filaments, we have two possible mechanisms in minds. In a series of papers, we claimed that they are formed as a consequence of the Kelvin-Helmholtz instabilities (Lugomer, 1999;Fukumoto and Lugomer, 2003). In this case, loops on the filament can be interpreted as loop solitons (Hasimoto, 1972), representing one dimensional soliton lattice.…”
Section: Introductionmentioning
confidence: 99%
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