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Untitled - Cdm.unimo.it

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Orthogonal<strong>it</strong>y 33<br />

only mention the relation existing between some Jacobi polynomials and Chebyshev<br />

polynomials, namely<br />

(2.6.1) P (α,α)<br />

n<br />

×<br />

k=0<br />

=<br />

<br />

Γ(2α + 1) Γ(n + α + 1)<br />

Γ(α + 1) Γ(n + 2α + 1)<br />

n Γ(k + α + 1<br />

2<br />

<br />

1 Γ(α + 2 ) 2<br />

k! (n − k)!<br />

) Γ(n − k + α + 1<br />

2 )<br />

T |n−2k|<br />

<br />

, n ∈ N, α > − 1<br />

2 .<br />

A problem related to the previous one, is the determination of the weighted norm<br />

of a polynomial, when the expansion coefficients, corresponding to a basis orthogonal<br />

w<strong>it</strong>h respect to another weight function, are known. We give an example. Sometimes,<br />

in practical applications <strong>it</strong> is useful to evaluate the integral 1<br />

−1 p2 dx, p ∈ Pn. If<br />

p is known in terms of <strong>it</strong>s Legendre coefficients, (2.3.6) is the formula we are looking<br />

for. The s<strong>it</strong>uation becomes more complicated when p is given in terms of the Fourier<br />

coefficients of another basis, say the Chebyshev basis. Let us assume that<br />

(2.6.2) p =<br />

Then<br />

(2.6.3)<br />

1<br />

−1<br />

p 2 dx =<br />

n<br />

k=0<br />

ckTk.<br />

The help of some trigonometry leads to the formula<br />

(2.6.4) Ikj =<br />

n n<br />

ckcjIkj,<br />

1<br />

where Ikj = TkTj dx.<br />

k=0 j=0<br />

−1<br />

π<br />

0<br />

cos kθ cos jθ sinθ dθ<br />

⎧<br />

⎪⎨<br />

0 if k + j is odd,<br />

=<br />

⎪⎩<br />

1 1<br />

+<br />

1 − (k + j) 2 1 − (k − j) 2 if k + j is even.

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