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21: 18.21 Hahn Class: Interrelations
Charlier Hermite
18.21.9 lim a ( 2 a ) 1 2 n C n ( ( 2 a ) 1 2 x + a ; a ) = ( 1 ) n H n ( x ) .
Meixner–Pollaczek Hermite
See accompanying text
Figure 18.21.1: Askey scheme. The number of free real parameters is zero for Hermite polynomials. … Magnify
22: 18.9 Recurrence Relations and Derivatives
Table 18.9.1: Classical OP’s: recurrence relations (18.9.1).
p n ( x ) A n B n C n
Table 18.9.2: Classical OP’s: recurrence relations (18.9.2_1).
p n ( x ) a n b n c n
Hermite
18.9.25 d d x H n ( x ) = 2 n H n 1 ( x ) ,
18.9.27 d d x 𝐻𝑒 n ( x ) = n 𝐻𝑒 n 1 ( x ) ,
23: 13.18 Relations to Other Functions
Hermite Polynomials
13.18.14 M 1 4 + n , 1 4 ( z 2 ) = ( 1 ) n n ! ( 2 n ) ! e 1 2 z 2 z H 2 n ( z ) ,
13.18.15 M 3 4 + n , 1 4 ( z 2 ) = ( 1 ) n n ! ( 2 n + 1 ) ! e 1 2 z 2 z 2 H 2 n + 1 ( z ) ,
13.18.16 W 1 4 + 1 2 n , 1 4 ( z 2 ) = 2 n e 1 2 z 2 z H n ( z ) .
24: 18.29 Asymptotic Approximations for q -Hahn and Askey–Wilson Classes
For a uniform asymptotic expansion of the Stieltjes–Wigert polynomials, see Wang and Wong (2006). For asymptotic approximations to the largest zeros of the q -Laguerre and continuous q 1 -Hermite polynomials see Chen and Ismail (1998).
25: 18.14 Inequalities
Hermite
Hermite
18.14.13 ( H n ( x ) ) 2 H n 1 ( x ) H n + 1 ( x ) , < x < .
Hermite
The successive maxima of | H n ( x ) | form a decreasing sequence for x 0 , and an increasing sequence for x 0 . …
26: 18.30 Associated OP’s
§18.30(iv) Associated Hermite Polynomials
The recursion relation for the associated Hermite polynomials, see (18.30.2), and (18.30.3), is
H 1 ( x ; c ) = 0 ,
H 0 ( x ; c ) = 1 ,
18.30.13 H n + 1 ( x ; c ) = 2 x H n ( x ; c ) 2 ( n + c ) H n 1 ( x ; c ) , n = 0 , 1 , .
27: 13.6 Relations to Other Functions
Hermite Polynomials
13.6.16 M ( n , 1 2 , z 2 ) = ( 1 ) n n ! ( 2 n ) ! H 2 n ( z ) ,
13.6.17 M ( n , 3 2 , z 2 ) = ( 1 ) n n ! ( 2 n + 1 ) ! 2 z H 2 n + 1 ( z ) ,
13.6.18 U ( 1 2 1 2 n , 3 2 , z 2 ) = 2 n z 1 H n ( z ) .
28: 18.12 Generating Functions
The z -radii of convergence will depend on x , and in first instance we will assume x [ 1 , 1 ] for Jacobi, ultraspherical, Chebyshev and Legendre, x [ 0 , ) for Laguerre, and x for Hermite. …
Hermite
18.12.15 e 2 x z z 2 = n = 0 H n ( x ) n ! z n ,
18.12.16 e x z 1 2 z 2 = n = 0 𝐻𝑒 n ( x ) n ! z n ,
18.12.17 1 + 2 x z + 4 z 2 ( 1 + 4 z 2 ) 3 2 exp ( 4 x 2 z 2 1 + 4 z 2 ) = n = 0 H n ( x ) n / 2 ! z n , | z | < 1 .
29: 18.28 Askey–Wilson Class
§18.28(vi) Continuous q -Hermite Polynomials
§18.28(vii) Continuous q 1 -Hermite Polynomials
For continuous q 1 -Hermite polynomials the orthogonality measure is not unique. …
From Continuous q -Ultraspherical to Continuous q -Hermite
From Continuous q -Hermite to Hermite
30: 18.16 Zeros
§18.16(v) Hermite
All zeros of H n ( x ) lie in the open interval ( 2 n + 1 , 2 n + 1 ) . … For an asymptotic expansion of x n , m as n that applies uniformly for m = 1 , 2 , , 1 2 n , see Olver (1959, §14(i)). … Lastly, in view of (18.7.19) and (18.7.20), results for the zeros of L n ( ± 1 2 ) ( x ) lead immediately to results for the zeros of H n ( x ) . …
Hermite