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We use a Hamiltonian normal form approach to study the dynamics of the water wave problem in the small amplitude long wave regime (KdV regime). If is the small parameter corresponding to the inverse of the wave length, we show that the normal form at order consists of two decoupled equation, one describing right going waves and the other describing left going waves. Performing a further non Hamiltonian transformation we conjugate each of these equations to a linear combination of the first three equations in the KdV hierarchy. At order we find nontrivial terms coupling the two counter-propagating waves.

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