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The Chebyshev polynomials Tn(x) can be written as Tn(x)=cos(ncos1x). (a) Verify that these functions do satisfy the Chebyshev equation. (b) Use de Moivre's theorem to show that an alternative expression is Tn(x)=revenn(1)r/2n!(nr)!r!xnr(1x2)r/2.

Short Answer

Expert verified
Verify derivatives satisfy Chebyshev equation, then expand Tn(x) using de Moivre's theorem and binomial expansion to get the alternative form.

Step by step solution

01

Understanding Chebyshev polynomials

Given the definition of the Chebyshev polynomials as Tn(x)=cos(ncos1x), first, recall the Chebyshev equation, which is (1x2)yxy+n2y=0.
02

Finding Derivatives of Tn(x)

Find the first and second derivatives of Tn(x). Use the chain rule to derive: y=nsin(ncos1x)11x2 and y=n(nsin2(ncos1x)11x2+cos(ncos1x)11x2).
03

Substitute Derivatives into the Chebyshev Equation

Substitute y, y, and y back into the Chebyshev equation: (1x2)yxy+n2y=0. Simplify each term to verify the equation holds.
04

Apply de Moivre's Theorem

Recall de Moivre's theorem which states that cos(nθ)=((cosθ+isinθ)n). Use this to express Tn(x)=cos(ncos1x) in terms of powers of x and trigonometric identities.
05

Expand Using Binomial Theorem

Expand (cos1x+isin(cos1x))n as a binomial series: Tn(x)=k=0n(nk)(isin(cos1x))k(cos(cos1x))nk.
06

Separate Real and Imaginary Parts

Extract the real part of the expansion by focusing on the even powers of i. This results in terms containing only x. Simplify each component to form the full expression.
07

Final Expression in Alternative Form

Combine terms according to whether the power of x is even. The final expression is: Tn(x)=r evenn(1)r/2n!(nr)!r!xnr(1x2)r/2.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Chebyshev equation
The Chebyshev equation is important in understanding the behavior of Chebyshev polynomials. The equation is given as (1x2)yxy+n2y=0 Here, y is a function of x, y is the first derivative of y, and y is the second derivative of y. Chebyshev polynomials, Tn(x), satisfy this differential equation. To verify that Tn(x)=cos(ncos1x) satisfies this equation, you first find the first and second derivatives of Tn(x). Then, substitute these derivatives into the equation. Simplify the terms to confirm that the equation holds true. This step-by-step differentiation and substitution help establish the relationship between Chebyshev polynomials and their governing differential equation. Understanding how to manipulate and work with this equation is key to both verifying the polynomial's properties and solving related differential equations.
de Moivre's Theorem
de Moivre's theorem links complex numbers and trigonometry, and it's vital for expanding Chebyshev polynomials in their alternative form. This theorem states: cos(nθ)=((cosθ+isinθ)n) Here, refers to the real part of the complex number. Using de Moivre's theorem, the Chebyshev polynomials can be rewritten in terms of powers of x. In the context of Chebyshev polynomials, we apply the theorem by starting with the given definition Tn(x)=cos(ncos1x). We then express cos(ncos1x) using de Moivre's theorem, which allows involving imaginary numbers. Though the expressions involve i, our interest lies in the real part, facilitating the transformation into a polynomial form.
Binomial Theorem
The binomial theorem is another critical tool in expressing Chebyshev polynomials in an alternative form. The binomial theorem states: (a+b)n=k=0n(nk)ankbk We use this theorem to expand (cos(cos1x)+isin(cos1x))n By treating acos(cos1x) and bisin(cos1x). This helps reframe our polynomial into a series involving powers of x. The resulting series contains both real and imaginary parts. We focus on extracting the real part to correlate directly with the Chebyshev polynomial. Breaking down this expansion into simpler sub-steps can solidify comprehension. Each term in the series combines different powers of x, refined in later steps.
Trigonometric Identities
Trigonometric identities simplify complex polynomial expressions, such as those found in Chebyshev polynomials. Some key identities include: - sin2(x)+cos2(x)=1 - cos(2x)=cos2(x)sin2(x) These identities help break down and simplify polynomials. For instance, when expressing Chebyshev polynomials in terms of x, trigonometric identities allow transforming and simplifying trigonometric terms like sin(cos1x) and cos(cos1x) directly into polynomial terms. Using known identities aids in combining or reducing terms, making complex expressions more manageable. For Chebyshev polynomial, converting trigonometric parts into powers of x leads to accessible, polynomial forms aiding in broader applications.

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Most popular questions from this chapter

In the quantum mechanical study of the scattering of a particle by a potential, a Born-approximation solution can be obtained in terms of a function y(r) that satisfies an equation of the form (2K2)y(r)=F(r) Assuming that yk(r)=(2π)3/2exp(ikr) is a suitably normalised eigenfunction of 2 corresponding to eigenvalue k2, find a suitable Green's function GK(r,r) By taking the direction of the vector rr as the polar axis for a k-space integration, show that GK(r,r) can be reduced to 14π|rr|wsinww2w02dw where w0=K|rr|. (This integral can be evaluated using a contour integration (chapter 20 ) to give (4π|rr|)1exp(iK|rr|).)

(a) Show that the equation y+aδ(x)y+λy=0 with y(±π)=0 and a real, has a set of eigenvalues λ satisfying tan(πλ)=2λa (b) Investigate the conditions under which negative eigenvalues, λ=μ2 with μ real, are possible.

The Laguerre polynomials, which are required for the quantum mechanical description of the hydrogen atom, can be defined by the generating function (equation (17.58)) G(x,h)=ehx/(1h)1h=n=0Ln(x)n!hn By differentiating the equation separately with respect to x and h, and resubstituting for G(x,h), prove that Ln and Ln(=dLn(x)/dx) satisfy the recurrence relations LnnLn1+nLn1=0Ln+1(2n+1x)Ln+n2Ln1=0 From these two equations and others derived from them, show that Ln(x) satisfies the Laguerre equation xLn+(1x)Ln+nLn=0.

Use the generating function for the Legendre polynomials Pn(x) to show that 01P2n+1(x)dx=(1)n(2n)!22n+1n!(n+1)! and that, except for the case n=0, 01P2n(x)dx=0.

(a) The differential operator L is defined by Ly=ddx(exdydx)exy4 Determine the eigenvalues λn of the problem $$ \mathcal{L} y_{n}=\lambda_{n} e^{x} y_{n} \quad 0

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