Chebyshev Polynomial of the Second Kind

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A modified set of Chebyshev polynomials defined by a slightly different generating function. They arise in the development of four-dimensional spherical harmonics in angular momentum theory. They are a special case of the Gegenbauer polynomial with alpha=1. They are also intimately connected with trigonometric multiple-angle formulas. The Chebyshev polynomials of the second kind are denoted U_n(x), and implemented in the Wolfram Language as ChebyshevU[n, x]. The polynomials U_n(x) are illustrated above for x in [-1,1] and n=1, 2, ..., 5.

The first few Chebyshev polynomials of the second kind are

U_0(x)=1
(1)
U_1(x)=2x
(2)
U_2(x)=4x^2-1
(3)
U_3(x)=8x^3-4x
(4)
U_4(x)=16x^4-12x^2+1
(5)
U_5(x)=32x^5-32x^3+6x
(6)
U_6(x)=64x^6-80x^4+24x^2-1.
(7)

When ordered from smallest to largest powers, the triangle of nonzero coefficients is 1; 2; -1, 4; -4, 8; 1, -12, 16; 6, -32, 32; ... (OEIS A053117).

The defining generating function of the Chebyshev polynomials of the second kind is

g(t,x)=1/(1-2xt+t^2)
(8)
=sum_(n=0)^(infty)U_n(x)t^n
(9)

for |x|<1 and |t|<1. To see the relationship to a Chebyshev polynomial of the first kind T(x), take partial/partialt of equation (9) to obtain

(partialg)/(partialt)=2(x-t)(1-2xt+t^2)^(-2)
(10)
=sum_(n=0)^(infty)nU_n(x)t^(n-1).
(11)

Multiplying (◇) by t then gives

 (2xt-2t^2)(1-2xt+t^2)^(-2)=sum_(n=0)^inftynU_n(x)t^n
(12)

and adding (12) and (◇) gives

((2xt-2t^2)+(1-2xt+t^2))/((1-2xt+t^2)^2)=(1-t^2)/((1-2xt+t^2)^2)
(13)
=sum_(n=0)^(infty)(n+1)U_n(x)t^n.
(14)

This is the same generating function as for the Chebyshev polynomial of the first kind except for an additional factor of 1-2xt+t^2 in the denominator.

The Rodrigues representation for U_n is

 U_n(x)=((-1)^n(n+1)sqrt(pi))/(2^(n+1)(n+1/2)!(1-x^2)^(1/2))(d^n)/(dx^n)[(1-x^2)^(n+1/2)].
(15)

The polynomials can also be defined in terms of the sums

U_n(x)=sum_(r=0)^(|_n/2_|)(-1)^r(n-r; r)(2x)^(n-2r)
(16)
=sum_(m=0)^(|_n/2_|)(n+1; 2m+1)x^(n-2m)(x^2-1)^m,
(17)

where |_x_| is the floor function and [x] is the ceiling function, or in terms of the product

 U_n(x)=2^nproduct_(k=1)^n[x-cos((kpi)/(n+1))]
(18)

(Zwillinger 1995, p. 696).

U_n(x) also obey the interesting determinant identity

 U_n=|2x 1 0 0 ... 0 0; 1 2x 1 0 ... 0 0; 0 1 2x 1 ... 0 0; 0 0 1 2x ... 0 0; 0 0 0 1 ... 1 0; | ... ... ... ... ... 1; 0 0 0 0 ... 1 2x|.
(19)

The Chebyshev polynomials of the second kind are a special case of the Jacobi polynomials P_n^((alpha,beta)) with alpha=beta=1/2,

U_n(x)=(n+1)(P_n^((1/2,1/2))(x))/(P_n^((1/2,1/2))(1))
(20)
=(n+1)_2F_1(-n,n+2;3/2;1/2(1-x)),
(21)

where _2F_1(a,b;c;x) is a hypergeometric function (Koekoek and Swarttouw 1998).

Letting x=costheta allows the Chebyshev polynomials of the second kind to be written as

 U_n(x)=(sin[(n+1)theta])/(sintheta).
(22)

The second linearly dependent solution to the transformed differential equation is then given by

 W_n(x)=(cos[(n+1)theta])/(sintheta),
(23)

which can also be written

 W_n(x)=(1-x^2)^(-1/2)T_(n+1)(x),
(24)

where T_n(x) is a Chebyshev polynomial of the first kind. Note that W_n(x) is therefore not a polynomial.

The triangle of resultants rho(U_n(x),U_k(x)) is given by {0}, {-4,0}, {0,-64,0}, {16,256,4096,0}, {0,0,0,1048576,0}, ... (OEIS A054376).

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