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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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are <strong>de</strong>voted to provi<strong>de</strong> a general one-to-one correspon<strong>de</strong>nce between completelyintegrable systems of analytic partial differential equations and theirassociated “submanifolds of solutions” (to be <strong>de</strong>fined precisely below) likeM above. Afterwards, we shall observe that conversely, the study of systemsof analytic partial differential equations also gains much informationfrom the direct study of their associated submanifolds of solutions.1492.3. Completely integrable systems of partial differential equations.Let now n, m, p ∈ N with n, m, p ≥ 1, let κ ∈ N with κ ≥ 2and let u = (u 1 , . . .,u m ) ∈ K m . Consi<strong>de</strong>r a collection of p multiindicesβ(1), . . ., β(p) ∈ N n with |β(q)| ≥ 1 for q = 1, . . .,p andmax 1≤q≤p |β(q)| = κ − 1. Consi<strong>de</strong>r also p integers j(1), . . ., j(p) with1 ≤ j(q) ≤ m for q = 1, . . ., p. Inspired by (7.28), we consi<strong>de</strong>r ageneral system of partial differential equations of n in<strong>de</strong>pen<strong>de</strong>nt variab<strong>les</strong>(x 1 , . . ., x n ) and m <strong>de</strong>pen<strong>de</strong>nt variab<strong>les</strong> (u 1 , . . .,u m ) which is of the followingform:()(E ) u j x α(x) = F αj x, u(x), (u j(q) (x))x β(q) 1≤q≤p ,where (j, α) ≠ (j(1), β(1)), . . ., (j(p), β(p)) and j = 1, . . .,m, |α| ≤ κ.Here, we assume that u = 0 is a local solution of the system (E ) and thatthe functions Fα j are K-algebraic or K-analytic in a neighbourhood of theorigin in K n+m+p . Among such systems are inclu<strong>de</strong>d ordinary differentialequations of any or<strong>de</strong>r κ ≥ 2, systems of second or<strong>de</strong>r partial differentialequation as studied in [24], etc.Throughout this article, we shall assume the system (E ) completely integrable.By analyzing the application of the Frobenius theorem in jet spaces,one can show (we will not <strong>de</strong>velop this) that the general solution of the system(E ) is given by u(x) := Ω(x, ν, χ), where the parameters ν ∈ K nand χ ∈ K n essentially correspond to the “initial conditions” u(0) and(u j(q) (0))x β(q) 1≤q≤p , and Ω is a K-analytic K n -valued mapping. In the case ofa generic submanifold as in Subsection 2.2 above, we recover the mappingΘ. In the sequel, we shall use the following terminology: the coordinates(x, u) will be called the variab<strong>les</strong> and the coordinates (ν, χ) will be calledthe parameters or the initial conditions. In Subsection 2.5 below, we shallintroduce a certain duality where the rô<strong>les</strong> between variab<strong>les</strong> and parametersare exchanged.2.4. Associated submanifold of solutions. The existence of the functionΩ and the analogy with Subsection 2.2 leads us to introduce the submanifoldof solutions associated to the completely integrable system (E ), whichby <strong>de</strong>finition is the m-codimensional K-analytic submanifold of K n+2m+p ,

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