Existence Domains Of Rogue Waves In The Plane оє п With A 1 In

Existence Domains Of Rogue Waves In The Plane оє п With A 1 In Figure 1 shows the domains of rogue wave existence in the plane (ω, κ), for either the focusing or the defocusing regimes. surprisingly, expo nential soliton states exist in the complementary. Figure 1. existence domains of rogue waves in the plane (κ, ω) with a = 1 in the focusing regime (σ = 1) and defocusing regime (σ = − 1). the red dotted line denotes ω = 1 κ 1 κ 3; the green dashed line denotes ω = 1 κ; the black solid line denotes ω = 1 κ − 1 κ 3. reuse & permissions.

Existence Domains Of Rogue Waves In The Plane оє п With A 1 In Whereas in the defocusing regime rogue waves exist for ω in the range [1 κ,1 κ 1 (a2κ3)]. figure 1 shows the domains of rogue wave existence in the plane (ω,κ) for either the focusing or the defocusing regime. surprisingly, exponential soliton states exist in the complementary region of the (ω,κ). Figure 1 shows the domains of rogue wave existence in the plane (!; ), for either the focusing or the defocusing regimes. surprisingly, expo nential soliton states exist in the complementary region of the (!; ) plane (see ref. [14] for details on the prop erties of these nonlinear waves). figure 2 illustrates a typical example of rogue wave. Subsequently, numerical investigations have been reported by moslem et al. [45] for the generation of acoustic rogue waves in dusty plasma composed of negatively charged dust grains and nonextensive electrons and ions. later, wang et al. [46] have investigated the solitary waves and rogue waves in plasma featuring tsallis distribution plasma. Instability of nonlinear waves with respect to long perturbations is known to be a regular mechanism of large wave generation, known as rogue or freak waves [25], [26]. it has been stated in [27] , [28] based on a number of examples from integrable systems that rogue wave solutions are inseparably linked to the modulational instability.

Color Online One Case Of Six Rogue Wave Excitations On A Double Plane Subsequently, numerical investigations have been reported by moslem et al. [45] for the generation of acoustic rogue waves in dusty plasma composed of negatively charged dust grains and nonextensive electrons and ions. later, wang et al. [46] have investigated the solitary waves and rogue waves in plasma featuring tsallis distribution plasma. Instability of nonlinear waves with respect to long perturbations is known to be a regular mechanism of large wave generation, known as rogue or freak waves [25], [26]. it has been stated in [27] , [28] based on a number of examples from integrable systems that rogue wave solutions are inseparably linked to the modulational instability. A \((3 1)\) dimensional nonlinear schrödinger (nls) equation that governs the evolution of the ea rogue waves in the current plasma system is derived through derivative expansion method. the existence domains for the first and second order rogue waves are investigated. Ic wave solution with nontrivial phase. this analytical expression generalizes the previous computations of the magnification factors of the constant amplitude wave, the dn . eriodic wave, and the cn periodic wave.fourth, we relate the existence of such rogue wave solutions to the modulation instability of the p.

A Rogue Wave Existence Condition On The A Q Plane Given By Eq 7 A \((3 1)\) dimensional nonlinear schrödinger (nls) equation that governs the evolution of the ea rogue waves in the current plasma system is derived through derivative expansion method. the existence domains for the first and second order rogue waves are investigated. Ic wave solution with nontrivial phase. this analytical expression generalizes the previous computations of the magnification factors of the constant amplitude wave, the dn . eriodic wave, and the cn periodic wave.fourth, we relate the existence of such rogue wave solutions to the modulation instability of the p.