Chapter 4 Linear Differential Operators
Chapter 4 Linear Differential Operators
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)