FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W4310769467> ?p ?o ?g. }

• W4310769467 endingPage "112963" @default.
• W4310769467 startingPage "112963" @default.
• W4310769467 abstract "The focus of this paper is on the dynamics of degenerate and non-degenerate vector solitons and their collision scenarios in the two-component long-wave–short-wave (2-LS) model of Newell type. The model equation that we study here governs the resonance interactions between two capillary waves (short waves) with a common gravity wave (long wave) for the surface wave of deep water. These degenerate and non-degenerate soliton solutions of the 2-LS model of Newell type are constructed via the bilinear KP-hierarchy reduction method and are expressed in forms of determinants. The degenerate solitons having only single-hump or single-valley profiles can undergo both elastic and inelastic collisions. Two particular types of degenerate solitons are also obtained, i.e., bound state solitons and V/Y-shaped solitons. The non-degenerate solitons and their collision scenarios have more interesting properties in contrast with the degenerate ones. The obvious one is that the non-degenerate one solitons possess symmetric or asymmetric double-hump and double-valley profiles if they propagate with identical velocities in all short-wave (SW) and long-wave (LW) components. Additionally, the soliton wavenumbers in the SW components and the LW component are unequal if the ones in the two SW components propagate with different velocities. The non-degenerate two solitons can undergo two different types of elastic collision scenarios in both SW and LW components: shape-preserving and shape-changing scenarios. We also study the collisions of non-degenerate solitons with degenerate ones, and find some intriguing properties. For instance, if the degenerate one soliton in one of the two SW components vanishes into background, then there is only one fundamental non-degenerate soliton in the corresponding SW component. However, this fundamental non-degenerate soliton still alters its profile from a symmetric double-hump waveform to an asymmetric double-hump one during its propagation process without interacting with other solitons. Furthermore, it is found a new class of soliton solutions referred to as (1,2,3) solitons. In these new types of soliton solutions, one SW component has only a single soliton, the other SW component has two solitons, whereas the LW component has three solitons." @default.
• W4310769467 created "2022-12-17" @default.
• W4310769467 creator A5011525444 @default.
• W4310769467 creator A5027043173 @default.
• W4310769467 creator A5069852316 @default.
• W4310769467 creator A5087981697 @default.
• W4310769467 date "2023-01-01" @default.
• W4310769467 modified "2023-10-09" @default.
• W4310769467 title "Degenerate and non-degenerate vector solitons and their interactions in the two-component long-wave–short-wave model of Newell type" @default.
• W4310769467 cites W102880676 @default.
• W4310769467 cites W1500925617 @default.
• W4310769467 cites W1507971731 @default.
• W4310769467 cites W1963640226 @default.
• W4310769467 cites W1964900659 @default.
• W4310769467 cites W1965579314 @default.
• W4310769467 cites W1971966778 @default.
• W4310769467 cites W1972276495 @default.
• W4310769467 cites W1973682626 @default.
• W4310769467 cites W1979655423 @default.
• W4310769467 cites W1981046457 @default.
• W4310769467 cites W1983326071 @default.
• W4310769467 cites W1985163664 @default.
• W4310769467 cites W1998898344 @default.
• W4310769467 cites W2000774502 @default.
• W4310769467 cites W2009501935 @default.
• W4310769467 cites W2015836561 @default.
• W4310769467 cites W2016199390 @default.
• W4310769467 cites W2019946394 @default.
• W4310769467 cites W2020083492 @default.
• W4310769467 cites W2026575824 @default.
• W4310769467 cites W2030839873 @default.
• W4310769467 cites W2031196196 @default.
• W4310769467 cites W2034576316 @default.
• W4310769467 cites W2036733217 @default.
• W4310769467 cites W2046107186 @default.
• W4310769467 cites W2050639649 @default.
• W4310769467 cites W2051000855 @default.
• W4310769467 cites W2055598066 @default.
• W4310769467 cites W2055790946 @default.
• W4310769467 cites W2069872719 @default.
• W4310769467 cites W2075585807 @default.
• W4310769467 cites W2080546069 @default.
• W4310769467 cites W2087920567 @default.
• W4310769467 cites W2089999622 @default.
• W4310769467 cites W2095669631 @default.
• W4310769467 cites W2102447842 @default.
• W4310769467 cites W2102691077 @default.
• W4310769467 cites W2135711634 @default.
• W4310769467 cites W2146325683 @default.
• W4310769467 cites W2149828519 @default.
• W4310769467 cites W2150850908 @default.
• W4310769467 cites W2316837428 @default.
• W4310769467 cites W2331580205 @default.
• W4310769467 cites W2596191334 @default.
• W4310769467 cites W2605049938 @default.
• W4310769467 cites W2800513532 @default.
• W4310769467 cites W2807706459 @default.
• W4310769467 cites W2865580628 @default.
• W4310769467 cites W2895686341 @default.
• W4310769467 cites W2917820707 @default.
• W4310769467 cites W2939603553 @default.
• W4310769467 cites W2963388978 @default.
• W4310769467 cites W2979929262 @default.
• W4310769467 cites W2983780142 @default.
• W4310769467 cites W2994516566 @default.
• W4310769467 cites W2994940566 @default.
• W4310769467 cites W2998385739 @default.
• W4310769467 cites W3016446181 @default.
• W4310769467 cites W3084534462 @default.
• W4310769467 cites W3101869306 @default.
• W4310769467 cites W3105667443 @default.
• W4310769467 cites W3110981200 @default.
• W4310769467 cites W3130557581 @default.
• W4310769467 cites W3133789907 @default.
• W4310769467 cites W3152670719 @default.
• W4310769467 cites W3182771134 @default.
• W4310769467 cites W4206917701 @default.
• W4310769467 cites W4220869105 @default.
• W4310769467 cites W4226020320 @default.
• W4310769467 cites W4283687445 @default.
• W4310769467 cites W4283801056 @default.
• W4310769467 cites W4286684985 @default.
• W4310769467 cites W4289550637 @default.
• W4310769467 cites W4289597960 @default.
• W4310769467 cites W4289711525 @default.
• W4310769467 cites W4294551609 @default.
• W4310769467 doi "https://doi.org/10.1016/j.chaos.2022.112963" @default.
• W4310769467 hasPublicationYear "2023" @default.
• W4310769467 type Work @default.
• W4310769467 citedByCount "3" @default.
• W4310769467 countsByYear W43107694672023 @default.
• W4310769467 crossrefType "journal-article" @default.
• W4310769467 hasAuthorship W4310769467A5011525444 @default.
• W4310769467 hasAuthorship W4310769467A5027043173 @default.
• W4310769467 hasAuthorship W4310769467A5069852316 @default.
• W4310769467 hasAuthorship W4310769467A5087981697 @default.
• W4310769467 hasConcept C109496249 @default.
• W4310769467 hasConcept C121332964 @default.

• next