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50 Polynomial Approximation of Differential Equations<br />

The set of the Chebyshev zeroes is the only distribution of Jacobi nodes for which<br />

the corresponding Gaussian weights are all the same. This further sets Chebyshev<br />

polynomials apart from the other families of orthogonal polynomials.<br />

Laguerre case - For α > −1 and n ≥ 1, we have<br />

(3.4.7) w (n)<br />

j<br />

Γ(n + α)<br />

= −<br />

n!<br />

This time the counterpart of (3.4.3) is<br />

(3.4.8)<br />

un(x)<br />

x − ξ (n)<br />

j<br />

<br />

L (α)<br />

n−1 (ξ(n) j ) d<br />

dx L(α) n (ξ (n)<br />

−1 j )<br />

= − 1<br />

n un−1(x) + qj(x), 1 ≤ j ≤ n,<br />

, 1 ≤ j ≤ n.<br />

where qj ∈ Pn−2, 1 ≤ j ≤ n, and un = L (α)<br />

n . The proof proceeds like that of the Jacobi<br />

case after recalling (2.2.13).<br />

Herm<strong>it</strong>e case - We have for n ≥ 1<br />

(3.4.9) w (n)<br />

j<br />

= √ π 2 n+1 n!<br />

<br />

H ′ n(ξ (n)<br />

−2 j ) , 1 ≤ j ≤ n.<br />

For the proof we can argue as in the previous cases. We only note that, by (1.7.8) one<br />

has H ′ n(ξ (n)<br />

j ) = 2nHn−1(ξ (n)<br />

j ), 1 ≤ j ≤ n.<br />

We observe that for all the cases the weights are strictly pos<strong>it</strong>ive. This is clear if<br />

we consider that<br />

w (n)<br />

j<br />

=<br />

n<br />

i=1<br />

[l (n)<br />

j ] 2 (ξ (n)<br />

i ) w (n)<br />

i<br />

=<br />

<br />

I<br />

[l (n)<br />

j ] 2 w dx > 0, 1 ≤ j ≤ n.<br />

Once the zeroes have been computed, the weights can be evaluated using the recurrence<br />

formula (1.1.2) to recover the values of un−1 and u ′ n.<br />

Due to their high accuracy, Gauss formulas play a fundamental role in the theoret-<br />

ical analysis of spectral methods. The possibil<strong>it</strong>y of integrating polynomials of degree<br />

2n − 1 just by knowing their values at n points will be widely used. The reader inter-<br />

ested in collecting more results may consult szegö(1939), stroud and secrest(1966),<br />

ghizzetti and ossicini(1970), davis and rabinow<strong>it</strong>z(1984), where other explic<strong>it</strong> ex-<br />

pressions of the weights are also given.

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