Under the constrained condition induced by the eigenfunction expression of the reflectionless potential
u=-2<
q,q>≡
f(
q), the Schr?dinger equation, the spatial part of the Lax pair of the
KdV equation, is nonlinearized to be a completely integrable system (R
2N ,
dpΛdq, H=F
0):
,
while the nonlinearization of the time part leads to its
N-involutive system {
F m}. The involutive solutions of the compatible system (
F0), (
Fm) are mapped by
f into the solutions of the
m-th
KdV equation.