Let u=u(x) be a smooth function that decays rapidly as ∣x∣→∞ and let L=−∂x2+u(x) denote the associated Schrödinger operator. Explain very briefly each of the terms appearing in the scattering data
S={{χn,cn}n=1N,R(k)},
associated with the operator L. What does it mean to say u(x) is reflectionless?
Given S, define the function
F(x)=n=1∑Ncn2e−χnx+2π1∫−∞∞eikxR(k)dk
If K=K(x,y) is the unique solution to the GLM equation
K(x,y)+F(x+y)+∫x∞K(x,z)F(z+y)dz=0
what is the relationship between u(x) and K(x,x) ?
Now suppose that u=u(x,t) is time dependent and that it solves the KdV equation ut+uxxx−6uux=0. Show that L=−∂x2+u(x,t) obeys the Lax equation
Lt=[L,A], where A=4∂x3−3(u∂x+∂xu).
Show that the discrete eigenvalues of L are time independent.
In what follows you may assume the time-dependent scattering data take the form
S(t)={{χn,cne4χn3t}n=1N,R(k,0)e8ik3t}.
Show that if u(x,0) is reflectionless, then the solution to the KdV equation takes the form
u(x,t)=−2∂x2∂2log[detA(x,t)]
where A is an N×N matrix which you should determine.
Assume further that R(k,0)=k2f(k), where f is smooth and decays rapidly at infinity. Show that, for any fixed x,
∫−∞∞eikxR(k,0)e8ik3t dk=O(t−1) as t→∞
Comment briefly on the significance of this result.
[You may assume detA1dxd(detA)=tr(A−1 dxdA) for a non-singular matrix A(x).]