Paper 2, Section II, B

Integrable Systems | Part II, 2009

Let L=x2+u(x,t)L=-\partial_{x}^{2}+u(x, t) be a Schrödinger operator and let AA be another differential operator which does not contain derivatives with respect to tt and such that

Lt=[L,A].L_{t}=[L, A] .

Show that the eigenvalues of LL are independent of tt, and deduce that if ff is an eigenfunction of LL then so is ft+Aff_{t}+A f. [You may assume that LL is self-adjoint.]

Let ff be an eigenfunction of LL corresponding to an eigenvalue λ\lambda which is nondegenerate. Show that there exists a function f^=f^(x,t,λ)\hat{f}=\hat{f}(x, t, \lambda) such that

Lf^=λf^,f^t+Af^=0.L \hat{f}=\lambda \hat{f}, \quad \hat{f}_{t}+A \hat{f}=0 .

Assume

A=x3+a1x+a0,A=\partial_{x}^{3}+a_{1} \partial_{x}+a_{0},

where ak=ak(x,t),k=0,1a_{k}=a_{k}(x, t), k=0,1 are functions. Show that the system ()(*) is equivalent to a pair of first order matrix PDEs

xF=UF,tF=VF\partial_{x} F=U F, \quad \partial_{t} F=V F

where F=(f^,xf^)TF=\left(\hat{f}, \partial_{x} \hat{f}\right)^{T} and U,VU, V are 2×22 \times 2 matrices which should be determined.

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