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Untitled - Cdm.unimo.it

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Special Families of Polynomials 9<br />

(1.4.8) |Pn(x)| ≤ 1<br />

<br />

π<br />

≤ 1<br />

<br />

π<br />

0<br />

π<br />

0<br />

π<br />

x 2 + (1 − x 2 ) cos 2 θ n/2 dθ<br />

2 2 2 1 + x<br />

x + (1 − x ) cos θ dθ = 2<br />

, x ∈ Ī, n ≥ 2.<br />

2<br />

This shows that the Legendre polynomials in<br />

parabolas y = − 1<br />

2 (1 + x2 ) and y = 1<br />

2 (1 + x2 ).<br />

1.5 Chebyshev polynomials<br />

Ī are uniformly bounded between the<br />

The Chebyshev polynomials (of the first kind) are related to the ultraspherical polyno-<br />

mials w<strong>it</strong>h α = β = −1 2 . In fact, they are defined by<br />

(− 1<br />

,− 1<br />

2 )<br />

2 (1.5.1) Tn := δn P n , n ∈ N,<br />

where<br />

δn := (n!2n ) 2<br />

(2n)! = n! √ π<br />

Γ(n + 1 =<br />

)<br />

2<br />

1−1<br />

n − 2 .<br />

n<br />

Consequently, they are solutions of the Sturm-Liouville problem<br />

(1.5.2) (1 − x 2 ) T ′′<br />

n − xT ′ n + n 2 Tn = 0 , n ∈ N.<br />

By taking α = β = − 1<br />

2<br />

formula<br />

in (1.3.8), after appropriate scaling, we arrive at the recursion<br />

(1.5.3) Tn(x) = 2xTn−1(x) − Tn−2(x) , x ∈<br />

where T0(x) = 1 and T1(x) = x.<br />

Ī , n ≥ 2,

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