Gegenbauer polynomials

E697761

Gegenbauer polynomials are a family of orthogonal polynomials on the interval [-1, 1] that generalize Legendre polynomials and play a key role in harmonic analysis and solutions of differential equations with spherical symmetry.

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Statements (46)

Predicate Object
instanceOf family of orthogonal polynomials
special functions
alsoKnownAs ultraspherical polynomials
associatedWith dimension parameter d via \lambda = (d-2)/2
belongTo Askey scheme of hypergeometric orthogonal polynomials NERFINISHED
definedOn interval [-1,1]
degree n in variable x
denotedBy C_n^{(\lambda)}(x) NERFINISHED
dependOn degree n
expressibleAs hypergeometric function {}_2F_1
field mathematics
generalize Chebyshev polynomials NERFINISHED
Legendre polynomials NERFINISHED
haveGeneratingFunction (1-2xt+t^2)^{-\lambda} = \sum_{n=0}^{\infty} C_n^{(\lambda)}(x) t^n
leadingCoefficient 2^n \frac{\Gamma(n+\lambda)}{n!\,\Gamma(\lambda)}
namedAfter Leopold Gegenbauer NERFINISHED
orthogonalityCondition \lambda > -1/2
orthogonalityIntegral \int_{-1}^1 (1-x^2)^{\lambda-1/2} C_m^{(\lambda)}(x) C_n^{(\lambda)}(x) dx = 0 for m \neq n
orthogonalOn [-1,1]
orthogonalWithRespectTo weight function (1-x^2)^{\lambda-1/2}
parameter \lambda
recurrenceRelation (n+1)C_{n+1}^{(\lambda)}(x) = 2(n+\lambda)x C_n^{(\lambda)}(x) - (n+2\lambda-1)C_{n-1}^{(\lambda)}(x)
relatedTo spherical harmonics on S^{d-1}
satisfy second-order linear differential equation
three-term recurrence relation
satisfyDifferentialEquation (1-x^2)y'' - (2\lambda+1)xy' + n(n+2\lambda)y = 0
specialCase Chebyshev polynomials of the first kind for \lambda = 0 (limit case) NERFINISHED
Chebyshev polynomials of the second kind for \lambda = 1 NERFINISHED
Legendre polynomials for \lambda = 1/2
subfield harmonic analysis
mathematical physics
orthogonal polynomials
special functions
symmetricProperty C_n^{(\lambda)}(-x) = (-1)^n C_n^{(\lambda)}(x)
usedFor addition theorems for spherical harmonics
expansion of powers of distance in higher dimensions
usedIn approximation theory
expansion of functions on spheres
harmonic analysis
potential theory
quantum mechanics with central potentials
solutions of differential equations with spherical symmetry
spectral methods for partial differential equations
valueAt C_n^{(\lambda)}(0) = 0 for odd n
C_n^{(\lambda)}(1) = \binom{n+2\lambda-1}{n}
C_{2k}^{(\lambda)}(0) = (-1)^k \frac{\Gamma(k+\lambda)}{k!\,\Gamma(\lambda)}

Referenced by (1)

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Jacobi polynomials generalizes Gegenbauer polynomials