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1: 18.31 Bernstein–Szegő Polynomials
Let ρ ( x ) be a polynomial of degree and positive when - 1 x 1 . …
2: 15.13 Zeros
If a , b , c , c - a , or c - b { 0 , - 1 , - 2 , } , then F ( a , b ; c ; z ) is not defined, or reduces to a polynomial, or reduces to ( 1 - z ) c - a - b times a polynomial. …
3: 18.34 Bessel Polynomials
Because the coefficients C n in (18.34.4) are not all positive, the polynomials y n ( x ; a ) cannot be orthogonal on the line with respect to a positive weight function. …
18.34.6 1 2 π i | z | = 1 z a - 2 y n ( z ; a ) y m ( z ; a ) e - 2 / z d z = ( - 1 ) n + a - 1 n !  2 a - 1 ( n + a - 2 ) ! ( 2 n + a - 1 ) δ n , m , a = 1 , 2 , ,
18.34.7 x 2 y n ′′ ( x ; a ) + ( a x + 2 ) y n ( x ; a ) - n ( n + a - 1 ) y n ( x ; a ) = 0 ,
18.34.8 lim α P n ( α , a - α - 2 ) ( 1 + α x ) P n ( α , a - α - 2 ) ( 1 ) = y n ( x ; a ) .
For uniform asymptotic expansions of y n ( x ; a ) as n in terms of Airy functions (§9.2) see Wong and Zhang (1997) and Dunster (2001c). …
4: 10.19 Asymptotic Expansions for Large Order
10.19.9 H ν ( 1 ) ( ν + a ν 1 3 ) H ν ( 2 ) ( ν + a ν 1 3 ) } 2 4 3 ν 1 3 e π i / 3 Ai ( e π i / 3 2 1 3 a ) k = 0 P k ( a ) ν 2 k / 3 + 2 5 3 ν e ± π i / 3 Ai ( e π i / 3 2 1 3 a ) k = 0 Q k ( a ) ν 2 k / 3 ,
10.19.13 H ν ( 1 ) ( ν + a ν 1 3 ) H ν ( 2 ) ( ν + a ν 1 3 ) } - 2 5 3 ν 2 3 e ± π i / 3 Ai ( e π i / 3 2 1 3 a ) k = 0 R k ( a ) ν 2 k / 3 + 2 4 3 ν 4 3 e π i / 3 Ai ( e π i / 3 2 1 3 a ) k = 0 S k ( a ) ν 2 k / 3 ,
5: 31.5 Solutions Analytic at Three Singularities: Heun Polynomials
31.5.2 Hp n , m ( a , q n , m ; - n , β , γ , δ ; z ) = H ( a , q n , m ; - n , β , γ , δ ; z )
is a polynomial of degree n , and hence a solution of (31.2.1) that is analytic at all three finite singularities 0 , 1 , a . …
6: 17.17 Physical Applications
In exactly solved models in statistical mechanics (Baxter (1981, 1982)) the methods and identities of §17.12 play a substantial role. … They were given this name because they play a role in quantum physics analogous to the role of Lie groups and special functions in classical mechanics. See Kassel (1995). A substantial literature on q -deformed quantum-mechanical Schrödinger equations has developed recently. It involves q -generalizations of exponentials and Laguerre polynomials, and has been applied to the problems of the harmonic oscillator and Coulomb potentials. …
7: 8.7 Series Expansions
8.7.6 Γ ( a , x ) = x a e - x n = 0 L n ( a ) ( x ) n + 1 , x > 0 .
8: 18.21 Hahn Class: Interrelations
C n ( x ; a ) = C x ( n ; a ) , n , x = 0 , 1 , 2 , .
18.21.6 lim N K n ( x ; N - 1 a , N ) = C n ( x ; a ) .
18.21.7 lim β M n ( x ; β , a ( a + β ) - 1 ) = C n ( x ; a ) .
18.21.9 lim a ( 2 a ) 1 2 n C n ( ( 2 a ) 1 2 x + a ; a ) = ( - 1 ) n H n ( x ) .
9: 1.11 Zeros of Polynomials
A polynomial of degree n with real or complex coefficients has exactly n real or complex zeros counting multiplicity. …A monic polynomial of even degree with real coefficients has at least two zeros of opposite signs when the constant term is negative. … The number of positive zeros of a polynomial with real coefficients cannot exceed the number of times the coefficients change sign, and the two numbers have same parity. … The discriminant of f ( z ) is defined by …The elementary symmetric functions of the zeros are (with a n 0 ) …
10: 35.4 Partitions and Zonal Polynomials
35.4.2 Z κ ( I ) = | κ | !  2 2 | κ | [ m / 2 ] κ 1 j < l ( κ ) ( 2 k j - 2 k l - j + l ) j = 1 ( κ ) ( 2 k j + ( κ ) - j ) !
Therefore Z κ ( T ) is a symmetric polynomial in the eigenvalues of T . …