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Chapter 4 Linear Differential Operators

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140 CHAPTER 4. LINEAR DIFFERENTIAL OPERATORS<br />

A solution with eigenvalue E = k2 and satisfying the boundary condition at<br />

r = 0 is<br />

<br />

A sin(kr), r < a,<br />

ψ(r) =<br />

(4.132)<br />

sin(kr + η), r > a.<br />

The conditions to be satisfied at r = a are:<br />

i) continuity, ψ(a − ɛ) = ψ(a + ɛ) ≡ ψ(a), and<br />

ii) jump in slope, −ψ ′ (a + ɛ) + ψ ′ (a − ɛ) + λψ(a) = 0.<br />

Therefore,<br />

ψ ′ (a + ɛ)<br />

ψ(a) − ψ′ (a − ɛ)<br />

= λ, (4.133)<br />

ψ(a)<br />

or<br />

Thus,<br />

and<br />

−π<br />

k cos(ka + η)<br />

sin(ka + η)<br />

− k cos(ka)<br />

sin(ka)<br />

= λ. (4.134)<br />

cot(ka + η) − cot(ka) = λ<br />

, (4.135)<br />

k<br />

η(k) = −ka + cot −1<br />

η(k)<br />

π 2π 3π 4π<br />

<br />

λ<br />

+ cot ka . (4.136)<br />

k<br />

Figure 4.4: The phase shift η(k) of equation (4.136) plotted against ka.<br />

A sketch of η(k) is shown in figure 4.4. The allowed values of k are required<br />

by the boundary condition<br />

ka<br />

sin(kR + η(k)) = 0 (4.137)

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