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Eigenvalue Analysis 163<br />

(8.2.19) (1 − x 2 ) r IV<br />

n,m(x) = n(n 2 − 1)(n + 2)ζn,mun(x) + {lower degree terms},<br />

where un = P (ν,ν)<br />

n . These relations can be checked by equating the coefficients of the<br />

monomials x n . W<strong>it</strong>h the same arguments used in section 3.8 (we recall for instance<br />

(3.8.12) and (3.8.15)), <strong>it</strong> is easy to show that<br />

(8.2.20)<br />

=<br />

1<br />

−1<br />

n<br />

i=0<br />

r IV<br />

n,m(η (n)<br />

i )¯rn,m(η (n)<br />

i ) ˜w (n)<br />

i<br />

r IV<br />

n,m¯rn,m w dx + (un 2 w,n − un 2 w) n(n 2 − 1)(n + 2)|ζn,m| 2 .<br />

Having unw,n ≥ unw, ∀n ≥ 1 (see (2.2.10) and (3.8.3)), integration by parts and<br />

formula (8.2.16) yield<br />

(8.2.21) Re<br />

n<br />

i=0<br />

1<br />

= Re r<br />

−1<br />

′′<br />

n,m(¯rn,mw) ′′ <br />

dx<br />

r IV<br />

n,m(η (n)<br />

i )¯rn,m(η (n)<br />

i ) ˜w (n)<br />

i<br />

≥ C<br />

1<br />

−1<br />

<br />

1<br />

≥ Re r<br />

−1<br />

IV<br />

<br />

n,m¯rn,mw dx<br />

|r ′′<br />

n,m| 2 w dx > 0, 1 ≤ m ≤ n − 1.<br />

We note that, since rn,m(±1) = r ′ n,m(±1) = 0, the last integral in (8.2.21) does not<br />

vanish (otherwise we would have rn,m ≡ 0). Hence, by (8.2.17) we deduce Reλn,m > 0,<br />

1 ≤ m ≤ n − 1.<br />

When ν = 0 (thus w ≡ 1), the right-hand side in (8.2.20) turns out to be real, after<br />

integrating by parts twice.<br />

Real and pos<strong>it</strong>ive eigenvalues are also observed for other values of the parameters<br />

α and β, and also for different type of boundary cond<strong>it</strong>ions such as those in (7.4.23).<br />

Hints for the determination of the characteristic polynomial are given in funaro and<br />

heinrichs(1990).

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