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21: 19.7 Connection Formulas
§19.7(i) Complete Integrals of the First and Second Kinds
E ( i k / k ) = ( 1 / k ) E ( k ) ,
E ( i k / k ) = ( 1 / k ) E ( k ) .
The second relation maps each hyperbolic region onto itself and each circular region onto the other: …
22: 10.38 Derivatives with Respect to Order
10.38.3 ( 1 ) n I ν ( z ) ν | ν = n = K n ( z ) + n ! 2 ( 1 2 z ) n k = 0 n 1 ( 1 ) k ( 1 2 z ) k I k ( z ) k ! ( n k ) ,
10.38.4 K ν ( z ) ν | ν = n = n ! 2 ( 1 2 z ) n k = 0 n 1 ( 1 2 z ) k K k ( z ) k ! ( n k ) .
I ν ( z ) ν | ν = 0 = K 0 ( z ) ,
K ν ( z ) ν | ν = 0 = 0 .
23: 10.31 Power Series
When ν is not an integer the corresponding expansion for K ν ( z ) is obtained from (10.25.2) and (10.27.4). …
10.31.1 K n ( z ) = 1 2 ( 1 2 z ) n k = 0 n 1 ( n k 1 ) ! k ! ( 1 4 z 2 ) k + ( 1 ) n + 1 ln ( 1 2 z ) I n ( z ) + ( 1 ) n 1 2 ( 1 2 z ) n k = 0 ( ψ ( k + 1 ) + ψ ( n + k + 1 ) ) ( 1 4 z 2 ) k k ! ( n + k ) ! ,
10.31.2 K 0 ( z ) = ( ln ( 1 2 z ) + γ ) I 0 ( z ) + 1 4 z 2 ( 1 ! ) 2 + ( 1 + 1 2 ) ( 1 4 z 2 ) 2 ( 2 ! ) 2 + ( 1 + 1 2 + 1 3 ) ( 1 4 z 2 ) 3 ( 3 ! ) 2 + .
24: 19.3 Graphics
See accompanying text
Figure 19.3.1: K ( k ) and E ( k ) as functions of k 2 for 2 k 2 1 . Graphs of K ( k ) and E ( k ) are the mirror images in the vertical line k 2 = 1 2 . Magnify
See accompanying text
Figure 19.3.4: E ( ϕ , k ) as a function of k 2 and sin 2 ϕ for 1 k 2 2 , 0 sin 2 ϕ 1 . If sin 2 ϕ = 1 ( k 2 ), then the function reduces to E ( k ) , with value 1 at k 2 = 1 . … Magnify 3D Help
See accompanying text
Figure 19.3.5: Π ( α 2 , k ) as a function of k 2 and α 2 for 2 k 2 < 1 , 2 α 2 2 . …As α 2 1 + it has the limit K ( k ) ( E ( k ) / k 2 ) . … Magnify 3D Help
See accompanying text
Figure 19.3.6: Π ( ϕ , 2 , k ) as a function of k 2 and sin 2 ϕ for 1 k 2 3 , 0 sin 2 ϕ < 1 . …Its value tends to as k 2 1 + by (19.6.6), and to the negative of the second lemniscate constant (see (19.20.22)) as k 2 ( = csc 2 ϕ ) 2 . Magnify 3D Help
25: 10.32 Integral Representations
10.32.6 K 0 ( x ) = 0 cos ( x sinh t ) d t = 0 cos ( x t ) t 2 + 1 d t , x > 0 .
10.32.17 K μ ( z ) K ν ( z ) = 2 0 K μ ± ν ( 2 z cosh t ) cosh ( ( μ ν ) t ) d t , | ph z | < 1 2 π .
10.32.18 K ν ( z ) K ν ( ζ ) = 1 2 0 exp ( t 2 z 2 + ζ 2 2 t ) K ν ( z ζ t ) d t t , | ph z | < π , | ph ζ | < π , | ph ( z + ζ ) | < 1 4 π .
For similar integrals for J ν ( z ) K ν ( z ) and I ν ( z ) K ν ( z ) see Paris and Kaminski (2001, p. 116). …
26: 10.39 Relations to Other Functions
10.39.2 K 1 2 ( z ) = K 1 2 ( z ) = ( π 2 z ) 1 2 e z .
10.39.4 K 3 4 ( z ) = 1 2 π 1 2 z 3 4 ( 1 2 U ( 1 , 2 z 1 2 ) + U ( 1 , 2 z 1 2 ) ) .
27: 14.6 Integer Order
14.6.8 Q ν m ( x ) = ( 1 ) m ( x 2 1 ) m / 2 x x Q ν ( x ) ( d x ) m .
28: 24.15 Related Sequences of Numbers
§24.15(iii) Stirling Numbers
The Stirling numbers of the first kind s ( n , m ) , and the second kind S ( n , m ) , are as defined in §26.8(i).
24.15.6 B n = k = 0 n ( 1 ) k k ! S ( n , k ) k + 1 ,
24.15.7 B n = k = 0 n ( 1 ) k ( n + 1 k + 1 ) S ( n + k , k ) / ( n + k k ) ,
24.15.9 p B n n S ( p 1 + n , p 1 ) ( mod p 2 ) , 1 n p 2 ,
29: Brian R. Judd
Judd’s books include Operator Techniques in Atomic Spectroscopy, published by McGraw-Hill in 1963 and reprinted by Princeton University Press in 1998, Second Quantization and Atomic Spectroscopy, published by Johns Hopkins in 1967, Topics in Atomic and Nuclear Theory (with J. …
30: 10.30 Limiting Forms
10.30.2 K ν ( z ) 1 2 Γ ( ν ) ( 1 2 z ) ν , ν > 0 ,
10.30.3 K 0 ( z ) ln z .
For K ν ( x ) , when ν is purely imaginary and x 0 + , see (10.45.2) and (10.45.7). … For K ν ( z ) see (10.25.3).