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

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70they consists of the seven partial differential relations (4.32), (4.33), (4.35),(4.37), (4.39), (4.43) and (4.45) below. At the end, we shall make the addition(4.47) below, producing the <strong>de</strong>sired subgoal (4.29) := (4.32) + (4.33)+ (4.35) + (4.37) + (4.39) + (4.43) + (4.45), with the numerotation of termscorresponding to the or<strong>de</strong>r of appearance of the terms of (4.29), as usual.Firstly, put j := k, l 1 := l 1 and l 2 := l 1 in (3.106):(4.31)0 = −2G k y + l 1 2δk l 1G l 1y + l 1 Hk l 1 ,x − δk l 1H l 1l1 ,x ++ 2 ∑ pG p L k l 1 ,p − 2δk l 1∑pG p L l 1l1 ,p − 1 2∑H p l 1Hp k + 1 ∑2 δk l 1ppH p l 1H l 1 p .∑Apply the operator 1 2 k Lk k,k (·) to the preceding equality, namely compute∑12 k Lk k,k · (4.31). This yields:(4.32)0 = − ∑ G k y l 1 Lk k,k + Gl 1y + 1 ∑H l 1 l k 2 1 ,x Lk k,k − 1 2 Hl 1l1 ,x Ll 1l1 ,l 1+kk+ ∑ ∑G p L k k,k Lk l 1 ,p − ∑ G p L l 1l1 ,l 1L k l 1 ,p − 1 ∑ ∑H p4l 1Hp k L k k,k +k ppk p+ 1 ∑H p4l 1H l 1 p L l 1l1 ,l 1.pSecondly, apply the operator − ∑ k Ll 2l2 ,k(·) to (4.32), namely compute− ∑ k Ll 2 · (4.32). This yields:(4.33)0 = 2 ∑ kl2 ,k− 2 ∑ k− 1 ∑2G k y l 1 Ll 2l2 ,k − 2Gl 1y l 1 Ll 2l2 ,l 1− ∑ kp∑pG p L l 2l2 ,k Lk l 1 ,p + 2 ∑ pH p l 1H l 1 p L l 2l2 ,l 1.H k l 1 ,x Ll 2l2 ,k + Hl 1l1 ,x Ll 2l2 ,l 1−G p L l 2l2 ,l 1L l 1l1 ,p + 1 2∑ ∑kpH p l 1H k p L l 2l2 ,k −Thirdly, put j := k, l 1 := l 2 and l 2 := l 1 with l 2 ≠ l 1 in (3.106):(4.34)0 = −2G k y + l 2 2δk l 2G l 1y + l 1 Hk l 2 ,x − δk l 2H l 1l1 ,x ++ 2 ∑ pG p L k l 2 ,p − 2δk l 2∑pG p L l 1l1 ,p − 1 2∑H p l 2Hp k + 1 ∑2 δk l 2ppH p l 1H l 1 p .

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