2009
DOI: 10.1063/1.3167806
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N = 2 supersymmetric extension of a hydrodynamic system in Riemann invariants

Abstract: In this paper, we formulate an N = 2 supersymmetric extension of a hydrodynamic-type system involving Riemann invariants. The supersymmetric version is constructed by means of a superspace and superfield formalism, using bosonic superfields, and consists of a system of partial differential equations involving both bosonic and fermionic variables. We make use of group-theoretical methods in order to analyze the extended model algebraically. Specifically, we calculate a Lie superalgebra of symmetries of our supe… Show more

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Cited by 1 publication
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“…5 When γ = 3, the equations represent the dispersionless limit of two non-interacting Korteweg-de Vries equations (known as Riemann invariants equations). 1,6,7 Finally, the γ = 4 case is the dispersionless limit of a Boussinesq equation. 8,9 In the context of hydrodynamic-type equations, other models have been supersymmetrized and analyzed from the group-theoretical point of view.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…5 When γ = 3, the equations represent the dispersionless limit of two non-interacting Korteweg-de Vries equations (known as Riemann invariants equations). 1,6,7 Finally, the γ = 4 case is the dispersionless limit of a Boussinesq equation. 8,9 In the context of hydrodynamic-type equations, other models have been supersymmetrized and analyzed from the group-theoretical point of view.…”
Section: Introductionmentioning
confidence: 99%
“…Examples of such models include the Korteweg-de Vries equation, 10,11 the Kadomtsev-Petviashvili equation, 12 the scalar Born-Infeld model, 13 a Gaussian fluid flow 14 and a hydrodynamic system expressed in terms of Riemann invariants. 6,7,15 The results are of interest since we can construct certain classes of solutions with the freedom of arbitrary functions of one or two arguments involving bosonic and fermionic variables.…”
Section: Introductionmentioning
confidence: 99%