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

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

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158such that every element (h, φ) ∈ Sym(M ), sufficiently close to thei<strong>de</strong>ntity mapping, may be represented by{ h(t) = Hκ0 (t, J κ 0t h(0)),(7.28)φ(τ) = Φ κ0 (τ, J κ 0τ φ(0)).Consequently, every element of Sym(M ) is uniquely <strong>de</strong>termined byits κ 0 -th jet at the origin and the dimension d of the <strong>Lie</strong> algebraSym(M ) is boun<strong>de</strong>d by the number of components of the vector(J κ 0t h(0), J κ 0τ φ(0)), namely we have(7.28)dim K Sym(E ) = dim K Sym(M ) ≤ (n+m) C κ 0n+m+κ 0+(m+p) C κ 0m+p+κ 0.(c) There exists ε ′ with 0 < ε ′ < ε and a K-algebraic or K-analytic mapping(H M , Φ M ) which may be constructed algorithmically by meansof the <strong>de</strong>fining equations of M , <strong>de</strong>fined in a neighbourhood of theorigin in K n+2m+p × K d with values in K n+2m+p and which satifies(H M (t, 0), Φ M (τ, 0)) ≡ (t, τ), such that every element (h, φ) ∈Sym(M ) <strong>de</strong>fined on the set {(t, τ) ∈ K n+2m+p : |t| < ε ′ , |τ| < ε ′ },sufficiently close to the i<strong>de</strong>ntity mapping and stabilizing M may berepresented as (h(t), φ(τ)) ≡ (H M (t, s h,φ ), Φ M (τ, s h,φ )) for a uniqueelement s h,φ ∈ K d <strong>de</strong>pending on the mapping (h, φ).(d) The mapping (t, τ, s) ↦−→ (H M (t, s), Φ M (τ, s)) <strong>de</strong>fines a local K-algebraic or K-analytic <strong>Lie</strong> group of local K-algebraic or K-analytictransformations stabilizing M .2.12. Applications. The proof of Theorem 6.4, which possesses strongsimilarities with the proof of Theorem 4.1 in [8], will not be presented.It seems that Theorem 6.4, together with the argumentation on the necessityof assumptions that M be solvable with respect to the variab<strong>les</strong> andthat its fundamental pair of foliations be covering, is a new result aboutthe finite-dimensionality of a completely integrable system of partial differentialequations having an arbitrary number of in<strong>de</strong>pen<strong>de</strong>nt and <strong>de</strong>pen<strong>de</strong>ntvariab<strong>les</strong>. The main interest lies in the fact that we obtain the algorithmicallyconstructible representation formula (7.28) together with the local <strong>Lie</strong> groupstructure mapping (H M , Φ M ). In particular, we get as a corollary that everytransformation (h(t), φ(τ)) given by a formal power series (not necessarilyconvergent) is as smooth as the applications (H κ0 , Φ κ0 ) are, namely everyformal element of Sym(M ) is necessarily K-algebraic or K-analytic. As acounterpart of its generality, Theorem 3 does not provi<strong>de</strong> optimal bounds,as shows the following illustration.Example 2.46. Let n = m = 1, let κ ≥ 3 and let (E ) <strong>de</strong>note the ordinarydifferential equation u x κ(x) = F(x, u(x), u x (x), . . .,u x κ−1(x)). Thenthe submanifold of solutions M is of the form u = ν + xχ 1 + · · · +

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