FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2962719814> ?p ?o ?g. }

• W2962719814 endingPage "94" @default.
• W2962719814 startingPage "49" @default.
• W2962719814 abstract "We investigate the quasi-integrability properties of various deformations of the Korteweg–de Vries (KdV) equation, depending on two parameters ε1 and ε2, which include among them the regularized long-wave (RLW) and modified regularized long-wave (mRLW) equations. We show, using analytical and numerical methods, that the charges, constructed from a deformation of the zero curvature equation for the KdV equation, are asymptotically conserved for various values of the deformation parameters. By this we mean that, despite the fact that the charges do vary in time during the scattering of solitons, they return after the scattering to the same values they had before it. This property was tested numerically for the scattering of two and three solitons, and analytically for the scattering of two solitons in the mRLW theory (ε2=ε1=1). In addition we show that for any values of ε1 and ε2 the Hirota method leads to analytical one-soliton solutions of our deformed equation but for ε1≠1 such solutions have the dispersion relation which depends on the parameter ε1. We also discuss some properties of soliton-radiation interactions seen in some of our simulations." @default.
• W2962719814 created "2019-07-30" @default.
• W2962719814 creator A5025034541 @default.
• W2962719814 creator A5058547513 @default.
• W2962719814 creator A5087272141 @default.
• W2962719814 date "2019-02-01" @default.
• W2962719814 modified "2023-09-25" @default.
• W2962719814 title "Quasi-integrability of deformations of the KdV equation" @default.
• W2962719814 cites W1966106671 @default.
• W2962719814 cites W1975881045 @default.
• W2962719814 cites W1979722387 @default.
• W2962719814 cites W1997644782 @default.
• W2962719814 cites W1999386091 @default.
• W2962719814 cites W2005380085 @default.
• W2962719814 cites W2011504998 @default.
• W2962719814 cites W2019585515 @default.
• W2962719814 cites W2020122483 @default.
• W2962719814 cites W2028044965 @default.
• W2962719814 cites W2028497428 @default.
• W2962719814 cites W2034131499 @default.
• W2962719814 cites W2043098860 @default.
• W2962719814 cites W2045576051 @default.
• W2962719814 cites W2050639649 @default.
• W2962719814 cites W2063222962 @default.
• W2962719814 cites W2077464783 @default.
• W2962719814 cites W2078790163 @default.
• W2962719814 cites W2080134171 @default.
• W2962719814 cites W2089996117 @default.
• W2962719814 cites W2115600080 @default.
• W2962719814 cites W2155566813 @default.
• W2962719814 cites W2179428325 @default.
• W2962719814 cites W2963092354 @default.
• W2962719814 cites W2963267222 @default.
• W2962719814 cites W2963580806 @default.
• W2962719814 cites W3011446994 @default.
• W2962719814 cites W3098850921 @default.
• W2962719814 cites W3102404994 @default.
• W2962719814 cites W3103923772 @default.
• W2962719814 cites W4253110154 @default.
• W2962719814 doi "https://doi.org/10.1016/j.nuclphysb.2018.12.004" @default.
• W2962719814 hasPublicationYear "2019" @default.
• W2962719814 type Work @default.
• W2962719814 sameAs 2962719814 @default.
• W2962719814 citedByCount "11" @default.
• W2962719814 countsByYear W29627198142020 @default.
• W2962719814 countsByYear W29627198142021 @default.
• W2962719814 countsByYear W29627198142022 @default.
• W2962719814 crossrefType "journal-article" @default.
• W2962719814 hasAuthorship W2962719814A5025034541 @default.
• W2962719814 hasAuthorship W2962719814A5058547513 @default.
• W2962719814 hasAuthorship W2962719814A5087272141 @default.
• W2962719814 hasBestOaLocation W29627198141 @default.
• W2962719814 hasConcept C121332964 @default.
• W2962719814 hasConcept C134306372 @default.
• W2962719814 hasConcept C146630112 @default.
• W2962719814 hasConcept C158622935 @default.
• W2962719814 hasConcept C177562468 @default.
• W2962719814 hasConcept C191486275 @default.
• W2962719814 hasConcept C195065555 @default.
• W2962719814 hasConcept C202579712 @default.
• W2962719814 hasConcept C2524010 @default.
• W2962719814 hasConcept C33923547 @default.
• W2962719814 hasConcept C37914503 @default.
• W2962719814 hasConcept C62520636 @default.
• W2962719814 hasConcept C74650414 @default.
• W2962719814 hasConcept C87651913 @default.
• W2962719814 hasConceptScore W2962719814C121332964 @default.
• W2962719814 hasConceptScore W2962719814C134306372 @default.
• W2962719814 hasConceptScore W2962719814C146630112 @default.
• W2962719814 hasConceptScore W2962719814C158622935 @default.
• W2962719814 hasConceptScore W2962719814C177562468 @default.
• W2962719814 hasConceptScore W2962719814C191486275 @default.
• W2962719814 hasConceptScore W2962719814C195065555 @default.
• W2962719814 hasConceptScore W2962719814C202579712 @default.
• W2962719814 hasConceptScore W2962719814C2524010 @default.
• W2962719814 hasConceptScore W2962719814C33923547 @default.
• W2962719814 hasConceptScore W2962719814C37914503 @default.
• W2962719814 hasConceptScore W2962719814C62520636 @default.
• W2962719814 hasConceptScore W2962719814C74650414 @default.
• W2962719814 hasConceptScore W2962719814C87651913 @default.
• W2962719814 hasFunder F4320320006 @default.
• W2962719814 hasFunder F4320320664 @default.
• W2962719814 hasFunder F4320320997 @default.
• W2962719814 hasLocation W29627198141 @default.
• W2962719814 hasLocation W29627198142 @default.
• W2962719814 hasLocation W29627198143 @default.
• W2962719814 hasLocation W29627198144 @default.
• W2962719814 hasLocation W29627198145 @default.
• W2962719814 hasOpenAccess W2962719814 @default.
• W2962719814 hasPrimaryLocation W29627198141 @default.
• W2962719814 hasRelatedWork W1634706908 @default.
• W2962719814 hasRelatedWork W1678195035 @default.
• W2962719814 hasRelatedWork W1982119754 @default.
• W2962719814 hasRelatedWork W2016664673 @default.
• W2962719814 hasRelatedWork W2025958831 @default.
• W2962719814 hasRelatedWork W2351869354 @default.
• W2962719814 hasRelatedWork W3017235236 @default.
• W2962719814 hasRelatedWork W3033777635 @default.

• next