Jost function

In scattering theory, the Jost function is the Wronskian of the regular solution and the (irregular) Jost solution to the differential equation $-\psi ''+V\psi =k^{2}\psi$ . It was introduced by Res Jost.

Background

We are looking for solutions $\psi (k,r)$ to the radial Schrödinger equation in the case $\ell =0$ ,

-\psi ''+V\psi =k^{2}\psi .

Regular and irregular solutions

A regular solution $\varphi (k,r)$ is one that satisfies the boundary conditions,

{\begin{aligned}\varphi (k,0)&=0\\\varphi _{r}'(k,0)&=1.\end{aligned}}

If $\int _{0}^{\infty }r|V(r)|<\infty$ , the solution is given as a Volterra integral equation,

\varphi (k,r)=k^{-1}\sin(kr)+k^{-1}\int _{0}^{r}dr'\sin(k(r-r'))V(r')\varphi (k,r').

We have two irregular solutions (sometimes called Jost solutions) $f_{\pm }$ with asymptotic behavior $f_{\pm }=e^{\pm ikr}+o(1)$ as $r\to \infty$ . They are given by the Volterra integral equation,

f_{\pm }(k,r)=e^{\pm ikr}-k^{-1}\int _{r}^{\infty }dr'\sin(k(r-r'))V(r')f_{\pm }(k,r').

If $k\neq 0$ , then $f_{+},f_{-}$ are linearly independent. Since they are solutions to a second order differential equation, every solution (in particular $\varphi$ ) can be written as a linear combination of them.

Jost function definition

The Jost function is

$\omega (k):=W(f_{+},\varphi )\equiv \varphi _{r}'(k,r)f_{+}(k,r)-\varphi (k,r)f_{+,x}'(k,r)$ ,

where W is the Wronskian. Since $f_{+},\varphi$ are both solutions to the same differential equation, the Wronskian is independent of r. So evaluating at $r=0$ and using the boundary conditions on $\varphi$ yields $\omega (k)=f_{+}(k,0)$ .