3.II.31E

Integrable Systems | Part II, 2006

The solution of the initial value problem of the KdV\mathrm{KdV} equation is given by

q(x,t)=−2ilim⁡k→∞k∂N∂x(x,t,k),q(x, t)=-2 i \lim _{k \rightarrow \infty} k \frac{\partial N}{\partial x}(x, t, k),

where the scalar function N(x,t,k)N(x, t, k) can be obtained by solving the following RiemannHilbert problem:

M(x,t,k)a(k)=N(x,t,−k)+b(k)a(k)exp⁡(2ikx+8ik3t)N(x,t,k),k∈R,\frac{M(x, t, k)}{a(k)}=N(x, t,-k)+\frac{b(k)}{a(k)} \exp \left(2 i k x+8 i k^{3} t\right) N(x, t, k), \quad k \in \mathbb{R},

M,NM, N and aa are the boundary values of functions of kk that are analytic for Im⁡k>0\operatorname{Im} k>0 and tend to unity as k→∞k \rightarrow \infty. The functions a(k)a(k) and b(k)b(k) can be determined from the initial condition q(x,0)q(x, 0).

Assume that MM can be written in the form

Ma=M(x,t,k)+cexp⁡(−2px+8p3t)N(x,t,ip)k−ip,Im⁡k⩾0,\frac{M}{a}=\mathcal{M}(x, t, k)+\frac{c \exp \left(-2 p x+8 p^{3} t\right) N(x, t, i p)}{k-i p}, \quad \operatorname{Im} k \geqslant 0,

where M\mathcal{M} as a function of kk is analytic for Im⁡k>0\operatorname{Im} k>0 and tends to unity as k→∞;ck \rightarrow \infty ; c and pp are constants and p>0p>0.

(a) By solving the above Riemann-Hilbert problem find a linear equation relating N(x,t,k)N(x, t, k) and N(x,t,ip)N(x, t, i p).

(b) By solving this equation explicitly in the case that b=0b=0 and letting c=2ipe−2x0c=2 i p e^{-2 x_{0}}, compute the one-soliton solution.

(c) Assume that q(x,0)q(x, 0) is such that a(k)a(k) has a simple zero at k=ipk=i p. Discuss the dominant form of the solution as t→∞t \rightarrow \infty and x/t=O(1)x / t=O(1).

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