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Travaux sur les symétries de Lie des équations aux ... - DMA - Ens

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154By <strong>de</strong>veloping the dual <strong>de</strong>fining functions of M with respect to the powersof χ, we may write(7.28) ν j = Ω ∗ j(χ, x, u) = ∑ γ∈N p χ γ Ω ∗ j,γ(x, u),where the functions Ω ∗ j,γ(x, u) are K-analytic in a neighbourhood of the origin,we may formulate a criterion for M to be non <strong>de</strong>generate with respectto the variab<strong>les</strong> (whose proof is skipped).Proposition 3.1. The submanifold M is not <strong>de</strong>generate with respect to thevariab<strong>les</strong> if and only if there exists an integer k such that the generic rank ofthe local K-analytic mapping(7.28) (x, u) ↦−→ ( Ω ∗ j,γ (x, u)) 1≤j≤m, γ∈N p , |γ|≤kis equal to n + m.Seeking for conditions which in<strong>sur</strong>e that Sym(M ) is finite-dimensional,it is therefore natural to assume that the generic rank of the mapping (7.28)is equal to n + m. Furthermore, to simplify the presentation, we shall assumethat the rank at (x, u) = (0, 0) (not only the generic rank) of themapping (7.28) is equal to n + m for k large enough. This is a “Zariskigeneric”assumption. Coming back to (7.28), we observe that this meansexactly that M is solvable with respect to the variab<strong>les</strong>. Then we <strong>de</strong>note byl ∗ 0 the smal<strong>les</strong>t integer k such that the rank at (x, u) = (0, 0) of the mapping(7.28) is equal to n + m and we say that M is l ∗ 0-solvable with respectto the variab<strong>les</strong>. Also, we <strong>de</strong>note by l 0 the integer max 1≤q≤p |β(q)| and wesay that M is l 0 -solvable with respect to the parameters.2.7. Fundamental isomorphism between Sym(E ) and Sym(M ). In theremain<strong>de</strong>r of this Section 2, we shall assume that M is l 0 -solvable withrespect to the parameters and l ∗ 0-solvable with respect to the variabes. Inthis case, viewing the variab<strong>les</strong> (ν 1 , . . .,ν m ) in the dual equations ν j =Ω ∗ j(χ, x, u) of M as a mapping of χ with (dual) “parameters” (x, u) andproceeding as in Subsection 2.2, we may construct a dual system of completelyintegrable partial differential equations of the form()(E ∗ ) ν j χ γ(χ) = Gj γ χ, ν(χ), (ν j(l) (χ))χ δ(l) 1≤l≤n ,where (j, γ) ≠ (j(1), δ(1)), . . ., (j(n), δ(n)). This system has its own infinitesimalsymmetry <strong>Lie</strong> algebra Sym(E ∗ ).Theorem 6.4. If M is both solvable with respect to the parameters andsolvable with respect to the variab<strong>les</strong>, we have the following two isomorphisms:(7.28) Sym(E ) ∼ = Sym(M ) ∼ = Sym(E ∗ ),

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