Lie-Bäcklund vector fields for the nonlinear system, \(Q_ t=AQ_{xx}+F(Q_ x,Q)\) (Q1085346)
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scientific article; zbMATH DE number 3981704
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Lie-Bäcklund vector fields for the nonlinear system, \(Q_ t=AQ_{xx}+F(Q_ x,Q)\) |
scientific article; zbMATH DE number 3981704 |
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Lie-Bäcklund vector fields for the nonlinear system, \(Q_ t=AQ_{xx}+F(Q_ x,Q)\) (English)
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1986
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We have analyzed the class of nonlinear second-order equations written as \(Q_ t=AQ_{xx}+F(Qx,Q)\) with \(Q=\left( \begin{matrix} u\\ v\end{matrix} \right)\) and A, F are, respectively, matrix and vector functions depending on Q, \(Q_ x\), from the point of view of Lie-Bäcklund vector fields. When the vector function F does not depend on \(Q_ x\), these equation set reduces to the coupled diffusion equations discussed by Steeb. But our generalized system encompasses a large class of physically meaning full nonlinear equations, such as (i) dispersive water waves and (ii) a completely anisotropic Heisenberg spin chain. We also exhibit a new nonlinear coupled system which do have nontrivial Lie-Bäcklund vector fields. Also our approach yields more information about the symmetry generators for a wider class of nonlinear equations than the function space approach of Fuchsteiner in a much simpler way.
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Lie-Bäcklund vector fields
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coupled diffusion equations
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full nonlinear equations
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dispersive water waves
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completely anisotropic Heisenberg spin chain
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symmetry generators
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0.8463229
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0.8373037
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0.81808496
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0.80523205
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0.8006904
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0.7928705
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0.7899679
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0.78741777
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