Chebyshev polynomials

Jordan Bell
December 7, 2016

1 First kind

On the one hand,

(cos⁡θ+i⁢sin⁡θ)n =∑0≤ν≤niν⁢(nν)⁢cosn-ν⁡θ⁢sinν⁡θ
=∑0≤2⁢k≤n(-1)k⁢(n2⁢k)⁢cosn-2⁢k⁡(θ)⁢sin2⁢k⁡(θ)
+i⁢∑0≤2⁢k+1≤n(-1)k⁢(n2⁢k+1)⁢cosn-2⁢k-1⁡(θ)⁢sin2⁢k+1⁡(θ).

On the other hand,

(cos⁡θ+i⁢sin⁡θ)n=(ei⁢θ)n=ei⁢n⁢θ=cos⁡n⁢θ+i⁢sin⁡n⁢θ.

Therefore

cos⁡n⁢θ =∑0≤k≤n/2(-1)k⁢(n2⁢k)⁢cosn-2⁢k⁡(θ)⁢sin2⁢k⁡(θ)
=∑0≤k≤n/2(-1)k⁢(n2⁢k)⁢cosn-2⁢k⁡(θ)⁢(1-cos2⁡θ)k
=∑0≤k≤n/2(n2⁢k)⁢cosn-2⁢k⁡(θ)⁢(cos2⁡θ-1)k
=∑0≤k≤n/2(n2⁢k)⁢cosn-2⁢k⁡(θ)⁢∑0≤j≤k(kj)⁢cos2⁢k-2⁢j⁡(θ)⁢(-1)j
=∑0≤j≤n/2(-1)j⁢cosn-2⁢j⁡(θ)⁢∑j≤k≤n/2(n2⁢k)⁢(kj).

Now,

∑j≤k≤n/2(n2⁢k)⁢(kj) =2n-2⁢j-1⁢(n-jj)⁢nn-j.

Hence

cos⁡n⁢θ=∑0≤j≤n/2(-1)j⁢cosn-2⁢j⁡(θ)⁢2n-2⁢j-1⁢(n-jj)⁢nn-j.

For z∈ℂ let

Tn⁢(z)=∑0≤j≤n/2(-1)j⁢2n-2⁢j-1⁢(n-jj)⁢nn-j⁢zn-2⁢j. (1)

Note

Tn⁢(z)⁢[zn]=2n-1⁢zn.
Theorem 1.
Tn⁢(cos⁡θ)=cos⁡(n⁢θ)

and

Tm∘Tn=Tm⁢n.
Proof.

For θ∈ℝ,

Tn⁢(cos⁡θ)=cos⁡(n⁢θ).

Then

Tm⁢(Tn⁢(cos⁡θ))=Tm⁢(cos⁡(n⁢θ))=cos⁡(m⁢n⁢θ)=Tm⁢n⁢(θ).

That is, for z∈[-1,1] we have Tm⁢(Tn⁢(z))=Tm⁢n⁢(z). Then by analytic continuation it follows that this is true for all z. ∎

Theorem 2.
Tn⁢(z)+Tn-2⁢(z)=2⁢z⁢Tn-1⁢(z).
Proof.

Using cos⁡(α+β)=cos⁡α⁢cos⁡β-sin⁡α⁢sin⁡β,

cos⁡(n⁢θ)=cos⁡(θ+(n-1)⁢θ)=cos⁡θ⁢cos⁡((n-1)⁢θ)-sin⁡θ⁢sin⁡((n-1)⁢θ)

and

cos⁡((n-2)⁢θ)=cos⁡(-θ+(n-1)⁢θ)=cos⁡θ⁢cos⁡((n-1)⁢θ)+sin⁡θ⁢sin⁡((n-1)⁢θ).

Then

cos⁡(n⁢θ)+cos⁡((n-2)⁢θ)=2⁢cos⁡θ⁢cos⁡((n-1)⁢θ).

Therefore

Tn⁢(cos⁡θ)+Tn-2⁢(cos⁡θ) =cos⁡(n⁢θ)+cos⁡((n-2)⁢θ)
=2⁢cos⁡θ⁢cos⁡((n-1)⁢θ)
=2⁢cos⁡θ⋅Tn-1⁢(cos⁡θ).

That is, for z∈[-1,1],

Tn⁢(z)+Tn-2⁢(z)=2⁢z⁢Tn-1⁢(z),

and by analytic continuation this is true for all z∈ℂ. ∎

2 Second kind

Define

n⁢Un-1⁢(z)=Tn′⁢(z). (2)
Theorem 3.
Un-1⁢(cos⁡θ)=sin⁡(n⁢θ)sin⁡θ

and

(1-z2)⁢Tn′′⁢(z)=n⁢Un⁢(z)-n⁢(n+1)⁢Tn⁢(z).
Proof.

On the one hand,

(Tn⁢(cos⁡θ))′ =-sin⁡θ⋅Tn′⁢(cos⁡θ).

On the other hand,

(Tn⁢(cos⁡θ))′=(cos⁡(n⁢θ))′=-n⁢sin⁡(n⁢θ).

Hence

Tn′⁢(cos⁡θ)=n⁢sin⁡(n⁢θ)sin⁡θ,Un-1⁢(cos⁡θ)=sin⁡(n⁢θ)sin⁡θ.

Now,

(Tn′⁢(cos⁡θ))′=-sin⁡θ⋅Tn′′⁢(cos⁡θ)

and

(Tn′⁢(cos⁡θ))′ =n⁢n⁢cos⁡(n⁢θ)⁢sin⁡θ-sin⁡(n⁢θ)⁢cos⁡θsin2⁡θ
=-n⁢cos⁡(n⁢θ)⁢sin⁡θ+sin⁡(n⁢θ)⁢cos⁡θsin2⁡θ+n⁢(n+1)⁢cos⁡(n⁢θ)⁢sin⁡θsin2⁡θ
=-n⁢sin⁡((n+1)⁢θ)sin2⁡θ+n⁢(n+1)⁢cos⁡(n⁢θ)sin⁡θ
=-n⁢Un⁢(cos⁡θ)sin⁡θ+n⁢(n+1)⁢Tn⁢(cos⁡θ)sin⁡θ.

Hence

Tn′′⁢(cos⁡θ)=n⁢Un⁢(cos⁡θ)sin2⁡θ-n⁢(n+1)⁢Tn⁢(cos⁡θ)sin2⁡θ

and then

Tn′′⁢(cos⁡θ)=n⁢Un⁢(cos⁡θ)1-cos2⁡θ-n⁢(n+1)⁢Tn⁢(cos⁡θ)1-cos2⁡θ.

By analytic continuation,

(1-z2)⁢Tn′′⁢(z)=n⁢Un⁢(z)-n⁢(n+1)⁢Tn⁢(z).

∎

Theorem 4.
Tn+1⁢(z)=z⁢Tn⁢(z)-(1-z2)⁢Un-1⁢(z).
Proof.
Tn+1⁢(cos⁡θ) =cos⁡(n⁢θ+θ)
=cos⁡(n⁢θ)⁢cos⁡θ-sin⁡(n⁢θ)⁢sin⁡θ
=Tn⁢(cos⁡θ)⁢cos⁡θ-Un-1⁢(cos⁡θ)⁢sin2⁡θ
=Tn⁢(cos⁡θ)⁢cos⁡θ-Un-1⁢(cos⁡θ)⁢(1-cos2⁡θ).

Therefore by analytic continuation,

Tn+1⁢(z)=z⁢Tn⁢(z)-(1-z2)⁢Un-1⁢(z).

∎

Theorem 5.
Un⁢(z)=Tn⁢(z)+z⁢Un-1⁢(z).
Proof.
Un⁢(cos⁡θ) =sin⁡(n⁢θ+θ)sin⁡θ
=cos⁡(n⁢θ)⁢sin⁡θ+cos⁡θ⁢sin⁡(n⁢θ)sin⁡θ
=Tn⁢(cos⁡θ)+cos⁡θ⋅Un-1⁢(cos⁡θ).

Therefore by analytic continuation,

Un⁢(z)=Tn⁢(z)+z⁢Un-1⁢(z).

∎

Theorem 6.
Un⁢(z)=2⁢z⁢Un-1⁢(z)+Un-2⁢(z).
Proof.

Using Theorem 4 and Theorem 5,

Un⁢(z) =Tn⁢(z)+z⁢Un-1⁢(z)
=z⁢Tn-1⁢(z)-(1-z2)⁢Un-2⁢(z)+z⁢Un-1⁢(z)
=z⁢[Un-1⁢(z)-z⁢Un-2⁢(z)]-(1-z2)⁢Un-2⁢(z)+z⁢Un-1⁢(z)
=2⁢z⁢Un-1⁢(z)+Un-2⁢(z).

∎

Theorem 7.
(1-z2)⁢Tn′′⁢(z)-z⁢Tn′⁢(z)+n2⁢Tn⁢(z)=0.
Proof.

Using Theorem 3, and Theorem 5,

(1-z2)⁢Tn′′⁢(z)-z⁢Tn′⁢(z)+n2⁢Tn⁢(z)=n⁢Un⁢(z)-n⁢(n+1)⁢Tn⁢(z)-n⁢z⁢Un-1⁢(z)+n2⁢Tn⁢(z)=n⁢(Tn⁢(z)+z⁢Un-1⁢(z))-n⁢(n+1)⁢Tn⁢(z)-n⁢z⁢Un-1⁢(z)+n2⁢Tn⁢(z)=0.

∎

From Theorem 1

Tn⁢(1)=Tn⁢(cos⁡0)=cos⁡(n⋅0)=1.

From Theorem 3,

Tn′⁢(1)=n⁢Un-1⁢(1)=n2.

Thus, Tn is the unique solution of the initial value problem

(1-x2)⁢y′′⁢(x)-x⁢y′⁢(x)+n2⁢y⁢(x)=0,y⁢(1)=1,y′⁢(1)=n2.
Theorem 8.
Tn⁢(z)2-(z2-1)⁢Un-1⁢(z)2=1.
Proof.

Using Theorem 1 and Theorem 3, for z=cos⁡θ,

Tn⁢(z)2-(z2-1)⁢Un-1⁢(z)2 =Tn⁢(cos⁡θ)2+(sin2⁡θ)⁢Un-1⁢(cos⁡θ)2
=cos2⁡(n⁢θ)+(sin2⁡θ)⁢sin2⁡(n⁢θ)sin2⁡θ
=cos2⁡(n⁢θ)+sin2⁡(n⁢θ)
=1.

By analytic continuation, this is true for all z. ∎

3 Inner products

For 0≤θ≤π let yn⁢(θ)=cos⁡(n⁢θ).

yn′′+n2⁢yn=0,yn′⁢(0)=0,yn′⁢(π)=0.
Theorem 9.
∫-11Tm⁢(x)⁢Tn⁢(x)1-x2⁢𝑑x=∫0πym⁢yn⁢𝑑θ=π2⋅δm,n.
Proof.

Let W=ym⁢yn′-yn⁢ym′. We calculate

W′ =ym′⁢yn′+ym⁢yn′′-yn′⁢ym′-yn⁢ym′′⁢ym⁢yn′′-yn⁢ym′′
=ym⁢yn′′-yn⁢ym′′
=ym⁢(-n2⁢yn)-yn⁢(-m2⁢ym)
=(m2-n2)⁢ym⁢yn.

Using W⁢(0)=0 and W⁢(π)=0,

∫0πW′⁢(θ)⁢𝑑θ=W⁢(π)-W⁢(0)=0.

Then

∫0π(m2-n2)⁢ym⁢yn⁢𝑑θ=0.

Doing the substitution ϕ=n⁢θ,

∫0πyn2⁢𝑑θ =∫0πcos2⁡(n⁢θ)⁢𝑑θ
=∫0π1+cos⁡(2⁢n⁢θ)2⁢𝑑θ
=π2.

Therefore

∫0πym⁢yn⁢𝑑θ=π2⋅δm,n.

For 0≤θ≤π, 1-cos2⁡θ=sin⁡θ. Then doing the substitution x=cos⁡θ, d⁢x=-sin⁡θ⁢d⁢θ,

∫0πym⁢yn⁢𝑑θ =∫0πcos⁡(m⁢θ)⁢cos⁡(n⁢θ)⁢𝑑θ
=∫0πcos⁡(m⁢θ)⁢cos⁡(n⁢θ)⁢-sin⁡θ⁢d⁢θ-sin⁡θ
=∫0πcos⁡(m⁢θ)⁢cos⁡(n⁢θ)-1-cos2⁡θ⁢(-sin⁡θ)⁢𝑑θ
=∫1-1Tm⁢(x)⁢Tn⁢(x)-1-x2⁢𝑑x
=∫-11Tm⁢(x)⁢Tn⁢(x)1-x2⁢𝑑x.

∎