Jost function explained

-\psi''+V\psi=k2\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=k2\psi.

Regular and irregular solutions

A regular solution

\varphi(k,r)

is one that satisfies the boundary conditions,

\begin{align} \varphi(k,0)&=0\\ \varphir'(k,0)&=1. \end{align}

If

infty
\int
0

r|V(r)|<infty

, the solution is given as a Volterra integral equation,

\varphi(k,r)=k-1\sin(kr)+k-1

rdr'\sin(k(r-r'))V(r')\varphi(k,r').
\int
0

There are two irregular solutions (sometimes called Jost solutions)

f\pm

with asymptotic behavior
\pmikr
f
\pm=e

+o(1)

as

r\toinfty

. They are given by the Volterra integral equation,
\pmikr
f
\pm(k,r)=e

-k-1

infty
\int
r

dr'\sin(k(r-r'))V(r')f\pm(k,r').

If

k\ne0

, 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\varphir'(k,r)f+(k,r)-\varphi(k,r)f+,r'(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)

.

Applications

The Jost function can be used to construct Green's functions for

\left[-\partial2
\partialr2

+V(r)-k2\right]G=-\delta(r-r').

In fact,

+(k;r,r')=-\varphi(k,r\wedger')f+(k,r\veer')
\omega(k)
G

,

where

r\wedger'\equivmin(r,r')

and

r\veer'\equivmax(r,r')

.

References