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11: 18.36 Miscellaneous Polynomials
These are OP’s on the interval ( 1 , 1 ) with respect to an orthogonality measure obtained by adding constant multiples of “Dirac delta weights” at 1 and 1 to the weight function for the Jacobi polynomials. … Orthogonality of the the classical OP’s with respect to a positive weight function, as in Table 18.3.1 requires, via Favard’s theorem, A n A n 1 C n > 0 for n 1 as per (18.2.9_5). … implying that, for n k , the orthogonality of the L n ( k ) ( x ) with respect to the Laguerre weight function x k e x , x [ 0 , ) . … Consider the weight functionand orthonormal with respect to the weight function
12: 18.25 Wilson Class: Definitions
§18.25(ii) Weights and Standardizations: Continuous Cases
18.25.2 0 p n ( x ) p m ( x ) w ( x ) d x = h n δ n , m .
18.25.4 w ( y 2 ) = 1 2 y | j Γ ( a j + i y ) Γ ( 2 i y ) | 2 ,
18.25.7 w ( y 2 ) = 1 2 y | j Γ ( a j + i y ) Γ ( 2 i y ) | 2 ,
18.25.15 h n = n ! ( N n ) ! ( γ + δ + 2 ) N N ! ( γ + 1 ) n ( δ + 1 ) N n .
13: 3.11 Approximation Techniques
§3.11(iii) Minimax Rational Approximations
Let f be continuous on a closed interval [ a , b ] and w be a continuous nonvanishing function on [ a , b ] : w is called a weight function. Then the minimax (or best uniform) rational approximation … w ( x ) being a given positive weight function, and again J n + 1 . Then (3.11.29) is replaced by …
14: 31.9 Orthogonality
31.9.5 1 2 ρ ( s , t ) w 1 ( s ) w 1 ( t ) w 2 ( s ) w 2 ( t ) d s d t = 0 , | n 1 n 2 | + | m 1 m 2 | 0 ,
31.9.6 ρ ( s , t ) = ( s t ) ( s t ) γ 1 ( ( s 1 ) ( t 1 ) ) δ 1 ( ( s a ) ( t a ) ) ϵ 1 ,
15: 31.10 Integral Equations and Representations
31.10.1 W ( z ) = C 𝒦 ( z , t ) w ( t ) ρ ( t ) d t
The weight function is given by
31.10.2 ρ ( t ) = t γ 1 ( t 1 ) δ 1 ( t a ) ϵ 1 ,
The weight function is
31.10.13 ρ ( s , t ) = ( s t ) ( s t ) γ 1 ( ( 1 s ) ( 1 t ) ) δ 1 ( ( 1 ( s / a ) ) ( 1 ( t / a ) ) ) ϵ 1 ,
16: 31.15 Stieltjes Polynomials
31.15.11 ( f , g ) ρ = Q f ( z ) g ( z ) ¯ ρ ( z ) d z ,
with weight function
31.15.12 ρ ( z ) = ( j = 1 N 1 k = 1 N | z j a k | γ k 1 ) ( j < k N 1 ( z k z j ) ) .
17: 18.38 Mathematical Applications
If the nodes in a quadrature formula with a positive weight function are chosen to be the zeros of the n th degree OP with the same weight function, and the interval of orthogonality is the same as the integration range, then the weights in the quadrature formula can be chosen in such a way that the formula is exact for all polynomials of degree not exceeding 2 n 1 . … The basic ideas of Gaussian quadrature, and their extensions to non-classical weight functions, and the computation of the corresponding quadrature abscissas and weights, have led to discrete variable representations, or DVRs, of Sturm–Liouville and other differential operators. …Each of these typically require a particular non-classical weight functions and analysis of the corresponding OP’s. …
Non-Classical Weight Functions
18: 18.30 Associated OP’s
with weight function with weight function
18.30.15 w ( x , c ) = | U ( c 1 2 , i x 2 ) | 2 .
with weight function
19: Bibliography R
  • W. P. Reinhardt (2021a) Erratum to:Relationships between the zeros, weights, and weight functions of orthogonal polynomials: Derivative rule approach to Stieltjes and spectral imaging. Computing in Science and Engineering 23 (4), pp. 91.
  • W. P. Reinhardt (2021b) Relationships between the zeros, weights, and weight functions of orthogonal polynomials: Derivative rule approach to Stieltjes and spectral imaging. Computing in Science and Engineering 23 (3), pp. 56–64.
  • 20: 18.35 Pollaczek Polynomials
    18.35.6 w ( λ ) ( cos θ ; a , b ) = π 1 e ( 2 θ π ) τ a , b ( θ ) ( 2 sin θ ) 2 λ 1 | Γ ( λ + i τ a , b ( θ ) ) | 2 , 0 < θ < π .
    18.35.6_1 ln ( w ( λ ) ( cos θ ; a , b ) ) = { 2 π ( a + b ) θ 1 + ( 2 λ 1 ) ln ( a + b ) + λ ln 4 + 2 ( a + b ) + O ( θ ) , θ 0 + , 2 π ( b a ) ( π θ ) 1 + ( 2 λ 1 ) ln ( a b ) + λ ln 4 + 2 ( a b ) + O ( π θ ) , θ π ,
    18.35.6_3 1 1 P n ( λ ) ( x ; a , b ) P m ( λ ) ( x ; a , b ) w ( λ ) ( x ; a , b ) d x + ζ D P n ( λ ) ( ζ ; a , b ) P m ( λ ) ( ζ ; a , b ) w ζ ( λ ) ( a , b ) = Γ ( 2 λ + n ) n ! ( λ + a + n ) δ n , m ,
    18.35.6_5 1 1 P n ( λ ) ( x ; a , b , c ) P m ( λ ) ( x ; a , b , c ) w ( λ ) ( x ; a , b , c ) d x = Γ ( c + 1 ) Γ ( 2 λ + c + n ) ( c + 1 ) n ( λ + a + c + n ) δ n , m ,
    18.35.6_6 w ( λ ) ( cos θ ; a , b , c ) = e ( 2 θ π ) τ a , b ( θ ) ( 2 sin θ ) 2 λ 1 | Γ ( c + λ + i τ a , b ( θ ) ) | 2 π | F ( 1 λ + i τ a , b ( θ ) , c c + λ + i τ a , b ( θ ) ; e 2 i θ ) | 2 ,