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

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234m for q = 1, . . ., p. In the present Part I, we study the <strong>Lie</strong> symmetries of ageneral system of analytic partial differential equations of the form:((E ) y j x α(x) = F αj x, y(x), ( y j(q) (x) ) ),x β(q) 1qpwhere j with 1 j m and α ∈ N n satisfy( ) ( ) ( )(1.2) j, α ≠ (j, 0) and j, α ≠ j(q), β(q) .In particular, all (κ + 1)-th partial <strong>de</strong>rivatives of the unknown y = y(x)<strong>de</strong>pend on a certain precise set of <strong>de</strong>rivatives of or<strong>de</strong>r κ: the system iscomplete. In addition, all the other partial <strong>de</strong>rivatives of or<strong>de</strong>r κ do also<strong>de</strong>pend on the same precise set of <strong>de</strong>rivatives.Here, we assume that u = 0 is a local solution of the system (E ) and thatthe functions Fα j are K-algebraic (in the sense of Nash) or K-analytic, in aneighborhood of the origin in K n+m+p . Even if our concern will be localthroughout, we will not introduce any special notation to speak of open subsetsand simply refer to various K µ . We will study five concrete instances,the first three ones being classical.Example 1.3. With n = m = κ = 1, a second or<strong>de</strong>r ordinary differentialequation(E 1 ) y xx = F(x, y, y x ),and more generally y x κ+1 = F(x, y, y x , . . .,y x κ), where x, y ∈ K,see [<strong>Lie</strong>1883, EL1890, Tr1896, Ca1924, Se1931, Ca1932a, Ol1986,Ar1988, BK1989, GTW1989, HK1989, Ib1992, Ol1995, N2003].Example 1.4. With n 2, m = 1 and κ = 1, a complete system of secondor<strong>de</strong>r equations(E 2 ) y x i 1x i 2 = F i1 ,i 2(x i , y, y x k), 1 i1 , i 2 n,see [Ha1937, Ch1975, Su2001] and Part III below.Example 1.5. Dually, with n = 1, m 2 and κ = 1, an ordinary system ofsecond or<strong>de</strong>r(E 3 ) yxx j = F j( x, y j 1), y j 1x , j = 1, . . ., m,see [Fe1995, Me2004] and the references therein.Example 1.6. With n = 1, m = 2 and κ = 1, a system of the form{y2x = F ( x, y 1 , y 2 , yx)1(E 4 )y 1 xx = G( x, y 1 , y 2 , y 1 x).

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