.
Chebyshev polynomials
In mathematics the Chebyshev polynomials, named after Pafnuty Chebyshev,[1] are a sequence of orthogonal polynomials which are related to de Moivre's formula and which can be defined recursively. One usually distinguishes between Chebyshev polynomials of the first kind which are denoted \( T_n \) and Chebyshev polynomials of the second kind which are denoted \(U_n \). The letter T is used because of the alternative transliterations of the name Chebyshev as Tchebycheff, Tchebyshev (French) or Tschebyschow (German).
The Chebyshev polynomials Tn or Un are polynomials of degree n and the sequence of Chebyshev polynomials of either kind composes a polynomial sequence.
Chebyshev polynomials are polynomials with the largest possible leading coefficient, but subject to the condition that their absolute value on the interval [-1,1] is bounded by 1. They are also the extremal polynomials for many other properties.[2]
Chebyshev polynomials are important in approximation theory because the roots of the Chebyshev polynomials of the first kind, which are also called Chebyshev nodes, are used as nodes in polynomial interpolation. The resulting interpolation polynomial minimizes the problem of Runge's phenomenon and provides an approximation that is close to the polynomial of best approximation to a continuous function under the maximum norm. This approximation leads directly to the method of Clenshaw–Curtis quadrature.
In the study of differential equations they arise as the solution to the Chebyshev differential equations
\( (1-x^2)\,y'' - x\,y' + n^2\,y = 0 \,\! \)
and
\( (1-x^2)\,y'' - 3x\,y' + n(n+2)\,y = 0 \,\! \)
for the polynomials of the first and second kind, respectively. These equations are special cases of the Sturm–Liouville differential equation.
Definition
The Chebyshev polynomials of the first kind are defined by the recurrence relation
\( \begin{align} T_0(x) & = 1 \\ T_1(x) & = x \\ T_{n+1}(x) & = 2xT_n(x) - T_{n-1}(x). \end{align} \)
The ordinary generating function for Tn is
\( \sum_{n=0}^{\infty}T_n(x) t^n = \frac{1-tx}{1-2tx+t^2}; \,\! \)
the exponential generating function is
\( \sum_{n=0}^{\infty}T_n(x) \frac{t^n}{n!} = \tfrac{1}{2}\left( e^{(x-\sqrt{x^2 -1})t}+e^{(x+\sqrt{x^2 -1})t}\right) = e^{tx} \cosh(t \sqrt{x^2-1}). \,\! \)
The generating function relevant for 2-dimensional potential theory and multipole expansion is
\( \sum\limits_{n=1}^{\infty }T_{n}\left( x\right) \frac{t^{n}}{n}=\ln \frac{1}{\sqrt{1-2tx+t^{2}}}. \)
The Chebyshev polynomials of the second kind are defined by the recurrence relation
\( \begin{align} U_0(x) & = 1 \\ U_1(x) & = 2x \\ U_{n+1}(x) & = 2xU_n(x) - U_{n-1}(x). \end{align} \)
The ordinary generating function for Un is
\( \sum_{n=0}^{\infty}U_n(x) t^n = \frac{1}{1-2 t x+t^2}; \,\! \)
the exponential generating function is
\( \sum_{n=0}^{\infty}U_n(x) \frac{t^n}{n!} = e^{tx} \left( \cosh(t \sqrt{x^2-1}) + \frac{x}{\sqrt{x^2-1}} \sinh(t \sqrt{x^2-1}) \right). \,\! \)
Trigonometric definition
The Chebyshev polynomials of the first kind can be defined as the unique polynomials satisfying
\( T_n(x)=\cos(n \arccos x)=\cosh(n\,\operatorname{arcosh}\,x) \,\! \)
or, in other words, as the unique polynomials satisfying
\( T_n(\cos(\vartheta))=\cos(n\vartheta) \,\! \)
for n = 0, 1, 2, 3, ... which is a variant (equivalent transpose) of Schröder's equation, viz. Tn(x) is functionally conjugate to nx, codified in the nesting property below. Further compare to the spread polynomials, in the section below.
The polynomials of the second kind satisfy:
\( U_n(\cos(\vartheta)) = \frac{\sin((n+1)\vartheta)}{\sin\vartheta} \, , \)
which is structurally quite similar to the Dirichlet kernel \( D_n(x) \,\!: \)
\( D_n(x) = \frac{\sin((2n+1)(x/2))}{\sin (x/2)} = U_{2n}(\cos (x/2))\, . \)
That cos(nx) is an nth-degree polynomial in cos(x) can be seen by observing that cos(nx) is the real part of one side of de Moivre's formula, and the real part of the other side is a polynomial in cos(x) and sin(x), in which all powers of sin(x) are even and thus replaceable through the identity cos2(x) + sin2(x) = 1.
This identity is quite useful in conjunction with the recursive generating formula, inasmuch as it enables one to calculate the cosine of any integral multiple of an angle solely in terms of the cosine of the base angle.
Evaluating the first two Chebyshev polynomials,
\( T_0(x)=\cos(0x) =1 \)
and
\( T_1(\cos(x))=\cos(x) \, , \)
one can straightforwardly determine that
\( \cos(2 \vartheta)=2\cos\vartheta \cos\vartheta - \cos(0 \vartheta) = 2\cos^{2}\,\vartheta - 1 \,\! \)
\( \cos(3 \vartheta)=2\cos\vartheta \cos(2\vartheta) - \cos\vartheta = 4\cos^3\,\vartheta - 3\cos\vartheta \, , \)
and so forth.
Two immediate corollaries are the composition identity (or nesting property specifying a semigroup)
\( T_n(T_m(x)) = T_{nm}(x)\, ; \)
and the expression of complex exponentiation in terms of Chebyshev polynomials: given z = a + bi,
\( \begin{align} z^n & = |z|^n \left(\cos \left(n\arccos \frac a{|z|}\right) + i \sin \left(n\arccos \frac a{|z|}\right)\right) \\ & = |z|^n T_n\left(\frac a{|z|}\right) + ib\ |z|^{n - 1}\ U_{n-1}\left(\frac a{|z|}\right). \end{align} \)
Pell equation definition
The Chebyshev polynomials can also be defined as the solutions to the Pell equation
\( T_n(x)^2 - (x^2-1) U_{n-1}(x)^2 = 1 \,\! \)
in a ring R[x].[3] Thus, they can be generated by the standard technique for Pell equations of taking powers of a fundamental solution:
\( T_n(x) + U_{n-1}(x) \sqrt{x^2-1} = (x + \sqrt{x^2-1})^n. \,\! \)
Products of Chebyshev polynomials
When working with Chebyshev polynomials quite often products of two of them occur. These products can be reduced to combinations of Chebyshev polynomials with lower or higher degree and concluding statements about the product are easier to make. It shall be assumed that in the following the index m is greater than or equal to the index n and n is not negative. For Chebyshev polynomials of the first kind the product expands to
\( 2 T_m(x) T_n(x) = T_{m+n}(x) + T_{|m-n|}(x) \)
which is an analogy to the addition theorem \( 2 \cos \alpha \cos \beta = \cos (\alpha + \beta) + \cos (\alpha - \beta) \) with the identities \( \alpha = m \arccos x, \beta = n \arccos x \) . For n=1 this results in the already known recurrence formula, just arranged differently, and with n=2 it forms the recurrence relation for all even or all odd Chebyshev polynomials (depending on the parity of the lowest m) which allows to design functions with prescribed symmetry properties. Three more useful formulas for evaluating Chebyshev polynomials can be concluded from this product expansion:
\( T_{2n}(x) = 2 T_n^2(x) - T_{0}(x) = 2 T_n^2(x) - 1 \)
\( T_{2n+1}(x) = 2 T_{n+1}(x) T_n(x) - T_1(x) = 2 T_{n+1}(x) T_n(x) - x \)
\( T_{2n-1}(x) = 2 T_{n-1}(x) T_n(x) - T_1(x) = 2 T_{n-1}(x) T_n(x) - x \)
For Chebyshev polynomials of the second kind products may be written as:
\( U_m(x) U_n(x) = \sum_{k=0}^{n} U_{m-n+2k}(x) = \sum_{p=m-n, step 2}^{m+n} U_{p}(x). \)
By this, like above, with n=2 the recurrence formula of Chebyshev polynomials of the second kind forms for both types of symmetry to
\( U_{m+2}(x) = U_2(x)U_m(x) - U_m(x) - U_{m-2}(x) = U_m(x)(U_2(x) - 1) - U_{m-2}(x) \) , depending on whether m starts with 2 or 3.
Relation between Chebyshev polynomials of the first and second kinds
The Chebyshev polynomials of the first and second kind are closely related by the following equations
\( \tfrac{d}{dx} \, T_n(x) = n U_{n-1}(x) \mbox{ , } n=1,\ldots \)
\( T_n(x) = \tfrac{1}{2} (U_n(x) - \, U_{n-2}(x)). \)
\( T_{n+1}(x) = xT_n(x) - (1 - x^2)U_{n-1}(x)\, \)
\( T_n(x) = U_n(x) - x \, U_{n-1}(x), \)
\( U_n(x) =2\sum_{j\,\, \text{odd}}^n T_j(x) \) , where n is odd.
\( U_n(x) =2\sum_{j\, \text{even}}^n T_j(x)-1 \) , where n is even.
The recurrence relationship of the derivative of Chebyshev polynomials can be derived from these relations
\( 2 T_n(x) = \frac{1}{n+1}\; \frac{d}{dx} T_{n+1}(x) - \frac{1}{n-1}\; \frac{d}{dx} T_{n-1}(x) \mbox{ , }\quad n=1,\ldots \)
This relationship is used in the Chebyshev spectral method of solving differential equations.
Equivalently, the two sequences can also be defined from a pair of mutual recurrence equations:
\( T_0(x) = 1\,\! \)
\( U_{-1}(x) = 0\,\! \)
\( T_{n+1}(x) = xT_n(x) - (1 - x^2)U_{n-1}(x)\, \)
\( U_n(x) = xU_{n-1}(x) + T_n(x)\, \)
These can be derived from the trigonometric formulae; for example, if \(x = \cos\vartheta \) , then
\( \begin{align} T_{n+1}(x) &= T_{n+1}(\cos(\vartheta)) \\ &= \cos((n + 1)\vartheta) \\ &= \cos(n\vartheta)\cos(\vartheta) - \sin(n\vartheta)\sin(\vartheta) \\ &= T_n(\cos(\vartheta))\cos(\vartheta) - U_{n-1}(\cos(\vartheta))\sin^2(\vartheta) \\ &= xT_n(x) - (1 - x^2)U_{n-1}(x). \\ \end{align} \)
Note that both these equations and the trigonometric equations take a simpler form if we, like some works, follow the alternate convention of denoting our \( U_n \) (the polynomial of degree n) with \( U_{n+1} \) instead.
Turán's inequalities for the Chebyshev polynomials are
\( T_n(x)^2-T_{n-1}(x) T_{n+1}(x)= 1-x^2>0 \text{ for } -1<x<1\! \) and
\( U_n(x)^2-U_{n-1}(x) U_{n+1}(x)= 1>0.\! \)
The integral relations are
\( \int_{-1}^1\frac{T_n(y)dy}{(y-x)\sqrt{1-y^2}} = \pi U_{n-1}(x), \)
\( \int_{-1}^1\frac{\sqrt{1-y^2}U_{n-1}(y)dy}{y-x} = -\pi T_n(x) \)
where integrals are considered as principal value.
Explicit expressions
Different approaches to defining Chebyshev polynomials lead to different explicit expressions such as:
\( T_n(x) = \begin{cases} \cos(n\arccos(x)) & \ |x| \le 1 \\ \cosh(n \, \operatorname{arcosh}(x)) & \ x \ge 1 \\ (-1)^n \cosh(n \, \operatorname{arcosh}(-x)) & \ x \le -1 \\ \end{cases} \)
\( \begin{align} T_n(x) & = \frac{\left (x-\sqrt{x^2-1} \right )^n + \left (x+\sqrt{x^2-1} \right )^n}{2} \\ & = \sum_{k=0}^{\left \lfloor \frac{n}{2} \right \rfloor} \binom{n}{2k} \left (x^2-1 \right )^k x^{n-2k} \\ & = x^n \sum_{k=0}^{\left \lfloor \frac{n}{2} \right \rfloor} \binom{n}{2k} \left (1 - x^{-2} \right )^k \\ & = \tfrac{n}{2} \sum_{k=0}^{\left \lfloor \frac{n}{2} \right \rfloor}(-1)^k \frac{(n-k-1)!}{k!(n-2k)!}~(2x)^{n-2k} && n>0 \\ & = n \sum_{k=0}^{n}(-2)^{k} \frac{(n+k-1)!} {(n-k)!(2k)!}(1 - x)^k && n>0 \\ & = {}_2F_1\left(-n,n;\tfrac 1 2; \tfrac{1}{2}(1-x)\right) \\ \end{align} \)
with inverse
\( x^n=2^{1-n}\mathop{{\sum}'}_{j=0, n-j\mathrm{even}}^n \binom{n}{(n-j)/2}T_j(x), \)
where the prime at the sum symbol indicates that the contribution of j=0 needs to be halved if it appears.
\( \begin{align} U_n(x) & = \frac{\left (x+\sqrt{x^2-1} \right )^{n+1} - \left (x-\sqrt{x^2-1} \right )^{n+1}}{2\sqrt{x^2-1}} \\ & = \sum_{k=0}^{\left \lfloor \frac{n}{2} \right \rfloor} \binom{n+1}{2k+1} \left (x^2-1 \right )^k x^{n-2k} \\ & = x^n \sum_{k=0}^{\left \lfloor \frac{n}{2} \right \rfloor} \binom{n+1}{2k+1} \left (1 - x^{-2} \right )^k \\ & = \sum_{k=0}^{\left \lfloor \frac{n}{2} \right \rfloor} \binom{2k-(n+1)}{k}~(2x)^{n-2k} && n>0 \\ & = \sum_{k=0}^{\left \lfloor \frac{n}{2} \right \rfloor} (-1)^k \binom{n-k}{k}~(2x)^{n-2k} && n>0 \\ & = \sum_{k=0}^{n}(-2)^{k} \frac{(n+k+1)!} {(n-k)!(2k+1)!}(1 - x)^k && n>0 \\ & = (n+1) \ {}_2F_1\left(-n,n+2; \tfrac{3}{2}; \tfrac{1}{2}(1-x) \right) \\ \end{align} \)
where 2F1 is a hypergeometric function.
Properties
Roots and extrema
A Chebyshev polynomial of either kind with degree n has n different simple roots, called Chebyshev roots, in the interval [−1,1]. The roots of the Chebyshev polynomial of the first kind are sometimes called Chebyshev nodes because they are used as nodes in polynomial interpolation. Using the trigonometric definition and the fact that
\( \cos\left((2k+1)\,\tfrac{\pi}{2}\right)=0 \)
one can easily prove that the roots of Tn are
\( x_k = \cos\left(\frac{2k-1}{2n}\pi\right),\quad k=1,\ldots,n. \)
Similarly, the roots of Un are
\( x_k = \cos\left(\frac{k}{n+1}\pi\right),\quad k=1,\ldots,n. \)
The extrema of Tn on the interval −1 ≤ x ≤ 1 are located at
\( x_k = \cos\left(\tfrac{k}{n}\pi\right),\quad k=0,\ldots,n. \)
One unique property of the Chebyshev polynomials of the first kind is that on the interval −1 ≤ x ≤ 1 all of the extrema have values that are either −1 or 1. Thus these polynomials have only two finite critical values, the defining property of Shabat polynomials. Both the first and second kinds of Chebyshev polynomial have extrema at the endpoints, given by:
\( T_n(1) = 1\, \)
\( T_n(-1) = (-1)^n\, \)
\( U_n(1) = n + 1\, \)
\( U_n(-1) = (n + 1)(-1)^n.\, \)
Differentiation and integration
The derivatives of the polynomials can be less than straightforward. By differentiating the polynomials in their trigonometric forms, it's easy to show that:
\( \frac{d T_n}{d x} = n U_{n - 1}\, \)
\( \frac{d U_n}{d x} = \frac{(n + 1)T_{n + 1} - x U_n}{x^2 - 1}\, \)
\( \frac{d^2 T_n}{d x^2} = n \frac{n T_n - x U_{n - 1}}{x^2 - 1} = n \frac{(n + 1)T_n - U_n}{x^2 - 1}.\, \)
The last two formulas can be numerically troublesome due to the division by zero (0/0 indeterminate form, specifically) at x = 1 and x = −1. It can be shown that:
\( \frac{d^2 T_n}{d x^2} \Bigg|_{x = 1} \!\! = \frac{n^4 - n^2}{3}, \)
\( \frac{d^2 T_n}{d x^2} \Bigg|_{x = -1} \!\! = (-1)^n \frac{n^4 - n^2}{3}. \)
Proof
Indeed, the following, more general formula holds:
\( \frac{d^p T_n}{d x^p} \Bigg|_{x = \pm 1} \!\! = (\pm 1)^{n+p}\prod_{k=0}^{p-1}\frac{n^2-k^2}{2k+1}. \)
This latter result is of great use in the numerical solution of eigenvalue problems.
\( \frac{d^p}{d x^p}T_n(x) = 2^p n\mathop{{\sum}'}_{k\ge 0, n-p-k \mathrm{even}}^{n-p} \binom{(n+p-k)/2-1}{(n-p-k)/2}\frac{[(n+p+k)/2-1]!}{[(n-p+k)/2]!}T_k(x),\quad p\ge 1, \)
where the prime at the summation symbols means that the term contributed by k=0 is to be halved, if it appears.
Concerning integration, the first derivative of the \(T_n \) implies that
\( \int U_n\, dx = \frac{T_{n + 1}}{n + 1}\, \)
and the recurrence relation for the first kind polynomials involving derivatives establishes that
\( \int T_n\, dx = \frac{1}{2} \left(\frac{T_{n + 1}}{n + 1} - \frac{T_{n - 1}}{n - 1}\right) = \frac{n T_{n + 1}}{n^2 - 1} - \frac{x T_n}{n - 1}.\, \)
Orthogonality
Both the \(T_n \) and the \(U_n \) form a sequence of orthogonal polynomials. The polynomials of the first kind are orthogonal with respect to the weight
\( \frac{1}{\sqrt{1-x^2}}, \,\! \)
on the interval [−1,1], i.e. we have:
\( \int_{-1}^1 T_n(x)T_m(x)\,\frac{dx}{\sqrt{1-x^2}}= \begin{cases} 0 &: n\ne m \\ \pi &: n=m=0\\ \pi/2 &: n=m\ne 0 \end{cases} \)
This can be proven by letting x = cos (θ) and using the defining identity Tn(cos (θ)) = cos (nθ).
Similarly, the polynomials of the second kind are orthogonal with respect to the weight
\( \sqrt{1-x^2} \,\! \)
on the interval [−1,1], i.e. we have:
\( \int_{-1}^1 U_n(x)U_m(x)\sqrt{1-x^2}\,dx = \begin{cases} 0 &: n\ne m, \\ \pi/2 &: n=m. \end{cases} \)
(Note that the measure \( \sqrt{1-x^2} \,dx \) is, to within a normalizing constant, the Wigner semicircle distribution).
The \(T_n \) also satisfy a discrete orthogonality condition:
\( \sum_{k=0}^{N-1}{T_i(x_k)T_j(x_k)} = \begin{cases} 0 &: i\ne j \\ N &: i=j=0 \\ N/2 &: i=j\ne 0 \end{cases} \,\! \)
where the \(x_k \) are the N Chebyshev nodes (see above) of \(T_N(x) \)
\( x_k=\cos\left(\pi\frac{2k+1}{2N}\right) . \)
For the polynomials of the second kind and with the same Chebyshev nodes \(x_k \) there are similar sums:
\( \sum_{k=0}^{N-1}{U_i(x_k)U_j(x_k)(1-x_k^2)} = \begin{cases} 0 &: i\ne j \\ N/2 &: i=j \end{cases} \,\! \)
and without the weight function:
\( \sum_{k=0}^{N-1}{U_i(x_k)U_j(x_k)} = \begin{cases} 0 &: parity(i)\ne parity(j) \\ N+N*min(i,j) &: parity(i)=parity(j) \\ \end{cases} \,\! \)
Based on the N zeros of the Chebyshev polynomial of the second kind \( U_N(x) \)
\( x_k=\cos\left(\pi\frac{k+1}{N+1}\right) \)
a different sum can be constructed
\( \sum_{k=0}^{N-1}{U_i(x_k)U_j(x_k)(1-x_k^2)} = \begin{cases} 0 &: i\ne j \\ \frac{N+1}{2} &: i=j \end{cases} \,\! \)
and again without the weight function:
\( \sum_{k=0}^{N-1}{U_i(x_k)U_j(x_k)} = \begin{cases} 0 &: parity(i)\ne parity(j) \\ (min(i,j)+1)(N-max(i,j)) &: parity(i)=parity(j) \\ \end{cases} \,\! \)
Minimal ∞-norm
For any given n ≥ 1, among the polynomials of degree n with leading coefficient 1,
\( f(x) = \frac1{2^{n-1}}T_n(x) \)
is the one of which the maximal absolute value on the interval [−1, 1] is minimal.
This maximal absolute value is
\( \frac1{2^{n-1}} \)
and |ƒ(x)| reaches this maximum exactly n + 1 times at
\( x = \cos \frac{k\pi}{n}\text{ for }0 \le k \le n. \)
Proof
Let's assume that \( w_n(x) \) is a polynomial of degree n with leading coefficient 1 with maximal absolute value on the interval [−1, 1] less than \( \frac1{2^{n-1}}. \)
Define
\( f_n(x) = \frac1{2^{n-1}}T_n(x) - w_n(x) \)
Because at extreme points of \( T_n \) we have \( |w_n(x)| < \left|\frac1{2^{n-1}}T_n(x)\right| \)
\( f_n(x) > 0 \text{ for } x = \cos \frac{2k\pi}{n} \text{ where } 0 \le 2k \le n \)
\( f_n(x) < 0 \text{ for } x = \cos \frac{(2k + 1)\pi}{n} \text{ where } 0 \le 2k + 1 \le n \)
From the intermediate value theorem, \( f_n(x) has at least n roots. However, this is impossible, as f_n(x) is a polynomial of degree n − 1, so the fundamental theorem of algebra implies it has at most n − 1 roots.
Other properties
The Chebyshev polynomials are a special case of the ultraspherical or Gegenbauer polynomials, which themselves are a special case of the Jacobi polynomials:
\( T_n(x)= \frac 1{{n-\frac 1 2 \choose n}} P_n^{-\frac 1 2, -\frac 1 2}(x)= \frac n 2 C_n^0(x), \)
\( U_n(x)= \frac 1{2{n+\frac 1 2 \choose n}} P_n^{\frac 1 2, \frac 1 2}(x)= C_n^1(x). \)
For every nonnegative integer n, Tn(x) and Un(x) are both polynomials of degree n. They are even or odd functions of x as n is even or odd, so when written as polynomials of x, it only has even or odd degree terms respectively. In fact,
\( T_{2n}(x)=T_n\left(2x^2-1\right)=2 T_n(x)^2-1 \)
and
\( 2 x U_n\left(1-2x^2\right)= (-1)^n U_{2n+1}(x). \)
The leading coefficient of \( T_n \) is 2n − 1 if 1 ≤ n, but 1 if 0 = n.
Tn are a special case of Lissajous curves with frequency ratio equal to n.
Several polynomial sequences like Lucas polynomials (\( L_n \)), Dickson polynomials (\( D_n \)), Fibonacci polynomials (\( F_n \)) are related to Chebyshev polynomials \( T_n \) and \( U_n \).
The Chebyshev polynomials of the first kind satisfy the relation
\( T_j(x) T_k(x) = \tfrac{1}{2}\left( T_{j+k}(x) + T_{|k-j|}(x)\right),\quad\forall j,k\ge 0,\, \)
which is easily proved from the product-to-sum formula for the cosine. The polynomials of the second kind satisfy the similar relation
\( T_j(x) U_k(x) = \begin{cases} \tfrac{1}{2}\left( U_{j+k}(x) + U_{k-j}(x)\right),\quad&\text{if } k\ge j-1.\\ \tfrac{1}{2}\left( U_{j+k}(x) + U_{j-k-2}(x)\right),\quad&\text{if } k\le j-2. \end{cases} \)
(with the convention \) U_{-1}\equiv 0 \) )
Similar to the formula
\( T_n\left(\cos\theta\right) = \cos(n \theta), \)
we have the analogous formula
\( T_{2n+1}\left(\sin\theta\right) = (-1)^n \sin((2n+1)\theta) . \)
For \( x\ne 0, \)
\( T_n\left(\dfrac{x+x^{-1}}2\right)=\dfrac{x^n+x^{-n}}2 and
x^n= T_n\left(\dfrac{x+x^{-1}}2\right)+ \dfrac{x-x^{-1}}2 U_{n-1}\left(\dfrac{x+x^{-1}}2\right), \)
which follows from the fact that this holds by definition for \( x = e^{i\theta}. \)
Let
\( C_n(x)=2T_n \left(\frac{x}{2}\right). \)
Then \( C_n(x) \) and \( C_m(x) \) are commuting polynomials:
\( C_n\left(C_m(x)\right)=C_m(C_n(x)), \)
as is evident in the Abelian nesting property specified above.
Generalized Chebyshev polynomials
The generalized Chebyshev polynomials \( T_a \) are defined by
\( T_a(\cos x)={}_2F_1\left(a,-a;\tfrac{1}{2};\tfrac{1}{2}(1-\cos x)\right)=\cos(a x), \)
where a is not necessarily an integer. They have the power series expansion
\( T_a(x)= \cos\left(\frac{\pi a}{2}\right)+ a \sum_{j=1}\frac{(2x)^j}{2j}\cos\left(\frac{\pi(a-j)}{2}\right){\frac{a+j-2}{2} \choose j-1}. \)
Examples
First kind
The first few Chebyshev polynomials of the first kind in the domain −1 < x < 1: The flat T0, T1, T2, T3, T4 and T5.
The first few Chebyshev polynomials of the first kind are OEIS A028297
\( T_0(x) = 1 \, \)
\( T_1(x) = x \, \)
\( T_2(x) = 2x^2 - 1 \, \)
\( T_3(x) = 4x^3 - 3x \, \)
\( T_4(x) = 8x^4 - 8x^2 + 1 \, \)
\( T_5(x) = 16x^5 - 20x^3 + 5x \, \)
\( T_6(x) = 32x^6 - 48x^4 + 18x^2 - 1 \, \)
\( T_7(x) = 64x^7 - 112x^5 + 56x^3 - 7x \, \)
\( T_8(x) = 128x^8 - 256x^6 + 160x^4 - 32x^2 + 1 \, \)
\( T_9(x) = 256x^9 - 576x^7 + 432x^5 - 120x^3 + 9x. \, \)
\( T_{10}(x) = 512x^{10} - 1280x^8 + 1120x^6 - 400x^4 + 50x^2-1. \, \)
\( T_{11}(x) = 1024x^{11} - 2816x^9 + 2816x^7 - 1232x^5 +220x^3 - 11x. \, \)
Second kind
The first few Chebyshev polynomials of the second kind in the domain −1 < x < 1: The flat U0, U1, U2, U3, U4 and U5. Although not visible in the image, Un(1) = n + 1 and Un(−1) = (n + 1)(−1)n.
The first few Chebyshev polynomials of the second kind are OEIS A053117
\( U_0(x) = 1 \, \)
\( U_1(x) = 2x \, \)
\( U_2(x) = 4x^2 - 1 \, \)
\( U_3(x) = 8x^3 - 4x \, \)
\( U_4(x) = 16x^4 - 12x^2 + 1 \, \)
\( U_5(x) = 32x^5 - 32x^3 + 6x \, \)
\( U_6(x) = 64x^6 - 80x^4 + 24x^2 - 1 \, \)
\( U_7(x) = 128x^7 - 192x^5 + 80x^3 - 8x \, \)
\( U_8(x) = 256x^8 - 448 x^6 + 240 x^4 - 40 x^2 + 1 \, \)
\( U_9(x) = 512x^9 - 1024 x^7 + 672 x^5 - 160 x^3 + 10 x. \, \)
As a basis set
The non-smooth function (top) y = −x3H(−x), where H is the Heaviside step function, and (bottom) the 5th partial sum of its Chebyshev expansion. The 7th sum is indistinguishable from the original function at the resolution of the graph.
In the appropriate Sobolev space, the set of Chebyshev polynomials form a orthonormal basis, so that a function in the same space can, on −1 ≤ x ≤ 1 be expressed via the expansion:[4]
\( f(x) = \sum_{n = 0}^\infty a_n T_n(x). \)
Furthermore, as mentioned previously, the Chebyshev polynomials form an orthogonal basis which (among other things) implies that the coefficients an can be determined easily through the application of an inner product. This sum is called a Chebyshev series or a Chebyshev expansion.
Since a Chebyshev series is related to a Fourier cosine series through a change of variables, all of the theorems, identities, etc. that apply to Fourier series have a Chebyshev counterpart.[4] These attributes include:
The Chebyshev polynomials form a complete orthogonal system.
The Chebyshev series converges to ƒ(x) if the function is piecewise smooth and continuous. The smoothness requirement can be relaxed in most cases — as long as there are a finite number of discontinuities in ƒ(x) and its derivatives.
At a discontinuity, the series will converge to the average of the right and left limits.
The abundance of the theorems and identities inherited from Fourier series make the Chebyshev polynomials important tools in numeric analysis; for example they are the most popular general purpose basis functions used in the spectral method,[4] often in favor of trigonometric series due to generally faster convergence for continuous functions (Gibbs' phenomenon is still a problem).
Example 1
Consider the Chebyshev expansion of \( \log(1+x) \) . One can express
\( \log(1+x) = \sum_{n = 0}^\infty a_n T_n(x). \)
One can find the coefficients a_n either through the application of an inner product or by the discrete orthogonality condition. For the inner product,
\( \int_{-1}^{+1}\frac{T_m(x)\log(1+x)}{\sqrt{1-x^2}}dx = \sum_{n=0}^{\infty}a_n\int_{-1}^{+1}\frac{T_m(x)T_n(x)}{\sqrt{1-x^2}}dx, \)
which gives
\( a_n= \begin{cases} -\log(2) &:n = 0 \\ \frac{-\pi(-1)^n}{n} &: n > 0. \end{cases}
Alternatively, when you cannot evaluate the inner product of the function you are trying to approximate, the discrete orthogonality condition gives
\( a_n=\frac{2-\delta_{0n}}{N}\sum_{k=0}^{N-1}T_n(x_k)\log(1+x_k), \)
where \( \delta_{ij} \) is the Kronecker delta function and the \( x_k \) are the N Gauss–Lobatto zeros of T_N(x)
\( x_k=\cos\left(\frac{\pi\left(k+\frac{1}{2}\right)}{N}\right) . \)
This allows us to compute the coefficients \( a_n \) very efficiently through the discrete cosine transform
\( a_n=\frac{2-\delta_{0n}}{N}\sum_{k=0}^{N-1}\cos\left(\frac{n\pi\left(k+\frac{1}{2}\right)}{N}\right)\log(1+x_k). \)
Example 2
To provide another example:
\( \begin{align}(1-x^2)^\alpha=& -\frac 1 {\sqrt \pi}\frac{\Gamma(\frac 1 2+\alpha)}{\Gamma(\alpha+1)}+ 2^{1-2\alpha} \sum_{n=0} (-1)^n {2\alpha \choose \alpha-n} T_{2n}(x)\\=& 2^{-2\alpha}\sum_{n=0} (-1)^n {2\alpha+1 \choose \alpha-n} U_{2n}(x).\end{align} \)
Partial sums
The partial sums of
\( f(x) = \sum_{n = 0}^\infty a_n T_n(x) \)
are very useful in the approximation of various functions and in the solution of differential equations (see spectral method). Two common methods for determining the coefficients an are through the use of the inner product as in Galerkin's method and through the use of collocation which is related to interpolation.
As an interpolant, the N coefficients of the (N − 1)th partial sum are usually obtained on the Chebyshev–Gauss–Lobatto[5] points (or Lobatto grid), which results in minimum error and avoids Runge's phenomenon associated with a uniform grid. This collection of points corresponds to the extrema of the highest order polynomial in the sum, plus the endpoints and is given by:
\( x_k = -\cos\left(\frac{k \pi}{N - 1}\right) ; \qquad \ k = 0, 1, \dots, N - 1. \)
Polynomial in Chebyshev form
An arbitrary polynomial of degree N can be written in terms of the Chebyshev polynomials of the first kind.[6] Such a polynomial p(x) is of the form
\( p(x) = \sum_{n=0}^{N} a_n T_n(x). \)
Polynomials in Chebyshev form can be evaluated using the Clenshaw algorithm.
Spread polynomials
The spread polynomials are in a sense equivalent to the Chebyshev polynomials of the first kind, but enable one to avoid square roots and conventional trigonometric functions in certain contexts, notably in rational trigonometry.
See also
Chebyshev filter
Chebyshev cube root
Dickson polynomials
Legendre polynomials
Hermite polynomials
Chebyshev rational functions
Approximation theory
The Chebfun system
Discrete Chebyshev transform
Markov brothers' inequality
Notes
Chebyshev polynomials were first presented in: P. L. Chebyshev (1854) "Théorie des mécanismes connus sous le nom de parallélogrammes," Mémoires des Savants étrangers présentés à l’Académie de Saint-Pétersbourg, vol. 7, pages 539–586.
Rivlin, Theodore J. The Chebyshev polynomials. Pure and Applied Mathematics. Wiley-Interscience [John Wiley & Sons], New York-London-Sydney,1974. Chapter 2, "Extremal Properties", pp. 56--123.
Jeroen Demeyer Diophantine Sets over Polynomial Rings and Hilbert's Tenth Problem for Function Fields, Ph.D. theses (2007), p.70.
Boyd, John P. (2001). Chebyshev and Fourier Spectral Methods (PDF) (second ed.). Dover. ISBN 0-486-41183-4.
Chebyshev Interpolation: An Interactive Tour
For more information on the coefficients, see: Mason, J. C. and Handscomb, D. C. (2002). Chebyshev Polynomials. Taylor & Francis.
References
Abramowitz, Milton; Stegun, Irene A., eds. (1965), "Chapter 22", Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, New York: Dover, p. 773, ISBN 978-0486612720, MR 0167642.
Dette, Holger (1995). "A Note on Some Peculiar Nonlinear Extremal Phenomena of the Chebyshev Polynomials". Proceedings of the Edinburgh Mathematical Society 38 (2): 343–355. doi:10.1017/S001309150001912X.
Elliott, David (1964). "The evaluation and estimation of the coefficients in the Chebyshev Series expansion of a function". Math. Comp. 18 (86): 274-284. doi:10.1090/S0025-5718-1964-0166903-7. MR 0166903.
Eremenko, A.; Lempert, L. (1994). "An Extremal Problem For Polynomials]" (PDF). Proceedings of the American Mathematical Society 122 (1): 191–193. doi:10.1090/S0002-9939-1994-1207536-1. MR 1207536.
Hernandez, M. A. (2001). "Chebyshev's approximation algorithms and applications". Comp. Math. Applic. 41: 433–445.
Mason, J. C. (1984). "Some properties and applications of Chebyshev polynomial and rational approximation". Lect. Not. Math. 1105: 27–48. doi:10.1007/BFb0072398.
Mason, J. C.; Handscomb, D. C. (2002). Chebyshev Polynomials. Taylor & Francis.
Mathar, R. J. (2006). "Chebyshev series expansion of inverse polynomials". J. Comput. Appl. Math. 196: 596–607. doi:10.1016/j.cam.2005.10.013.
Koornwinder, Tom H.; Wong, Roderick S. C.; Koekoek, Roelof; Swarttouw, René F. (2010), "Orthogonal Polynomials", in Olver, Frank W. J.; Lozier, Daniel M.; Boisvert, Ronald F.; Clark, Charles W., NIST Handbook of Mathematical Functions, Cambridge University Press, ISBN 978-0521192255, MR 2723248
Remes, Eugene. "On an Extremal Property of Chebyshev Polynomials" (PDF).
Salzer, Herbert E. (1976). "Converting interpolation series into Chebyshev Series by Recurrence Formulas". Math. Comp. 30 (134): 295–302. doi:10.1090/S0025-5718-1976-0395159-3. MR 0395159.
Scraton, R. E. (1969). "The Solution of integral equations in Chebyshev series". Math. Comput 23 (108): 837–844. doi:10.1090/S0025-5718-1969-0260224-4. MR 0260224.
Smith, Lyle B. (1966). "Algorithm 277, Computation of Chebyshev series coefficients". Comm. ACM 9 (2): 86–87. doi:10.1145/365170.365195.
Suetin, P. K. (2001), "C/c021940", in Hazewinkel, Michiel, Encyclopedia of Mathematics, Springer, ISBN 978-1-55608-010-4
Retrieved from "http://en.wikipedia.org/"
All text is available under the terms of the GNU Free Documentation License
