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Mathematical Methods for Physicists: A concise introduction - Site Map

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STURM±LIOUVILLE SYSTEMS<br />

the system. In general there is one eigenfunction to each eigenvalue. This is the<br />

non-degenerate case. In the degenerate case, more than one eigenfunction may<br />

correspond to the same eigenvalue. The eigenfunctions <strong>for</strong>m an orthogonal set<br />

with respect to the density function p…x† which is generally 0.Thus by suitable<br />

normalization the set of functions can be made an orthonormal set with respect to<br />

p…x† in a x b. We now proceed to prove these two general claims.<br />

Property 1<br />

If r…x† and q…x† are real, the eigenvalues of a Sturm±Liouville<br />

system are real.<br />

We start with the Sturm±Liouville equation (7.104) and the boundary conditions<br />

(7.104a):<br />

<br />

d dy<br />

r…x† ‡‰q…x†‡p…x†Šy ˆ 0; a x b;<br />

dx dx<br />

k 1 y…a†‡k 2 y 0 …a† ˆ0; l 1 y…b†‡l 2 y 0 …b† ˆ0;<br />

and assume that r…x†; q…x†; p…x†; k 1 ; k 2 ; l 1 ,andl 2 are all real, but and y may be<br />

complex. Now take the complex conjugates<br />

<br />

d d y<br />

r…x† ‡‰q…x†‡ p…x†Šy<br />

dx dx<br />

ˆ 0;<br />

…7:105†<br />

k 1 y…a†‡k 2 y 0 …a† ˆ0; l 1 y…b†‡l 2 y 0 …b† ˆ0;<br />

…7:105a†<br />

where y and are the complex conjugates of y and , respectively.<br />

Multiplying (7.104) by y, (7.105) by y, and subtracting, we obtain after<br />

simplifying<br />

d <br />

dx r…x†…yy 0 yy 0 <br />

† ˆ… †p…x†yy: <br />

Integrating from a to b, and using the boundary conditions (7.104a) and (7.105a),<br />

we then obtain<br />

… †<br />

Z b<br />

a<br />

p…x† y 0 2 dx ˆ r…x†…yy 0 yy 0 †j b a ˆ 0:<br />

Since p…x† 0ina x b, the integral on the left is positive and there<strong>for</strong>e<br />

ˆ , that is, is real.<br />

Property 2<br />

The eigenfunctions corresponding to two di€erent eigenvalues<br />

are orthogonal with respect to p…x† in a x b.<br />

341

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