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21: 10.42 Zeros
§10.42 Zeros
Properties of the zeros of I ν ( z ) and K ν ( z ) may be deduced from those of J ν ( z ) and H ν ( 1 ) ( z ) , respectively, by application of the transformations (10.27.6) and (10.27.8). For example, if ν is real, then the zeros of I ν ( z ) are all complex unless 2 < ν < ( 2 1 ) for some positive integer , in which event I ν ( z ) has two real zeros. … For z -zeros of K ν ( z ) , with complex ν , see Ferreira and Sesma (2008). …
22: 10.39 Relations to Other Functions
Elementary Functions
10.39.2 K 1 2 ( z ) = K 1 2 ( z ) = ( π 2 z ) 1 2 e z .
Parabolic Cylinder Functions
Confluent Hypergeometric Functions
Generalized Hypergeometric Functions and Hypergeometric Function
23: 28.28 Integrals, Integral Representations, and Integral Equations
§28.28(i) Equations with Elementary Kernels
D 0 ( ν , μ , z ) = M ν ( 3 ) ( z ) M μ ( 4 ) ( z ) M ν ( 4 ) ( z ) M μ ( 3 ) ( z ) ,
§28.28(iv) Integrals of Products of Mathieu Functions of Integer Order
Ds 0 ( n , m , z ) = Ms n ( 3 ) ( z ) Ms m ( 4 ) ( z ) Ms n ( 4 ) ( z ) Ms m ( 3 ) ( z ) ,
§28.28(v) Compendia
24: 28.25 Asymptotic Expansions for Large z
§28.25 Asymptotic Expansions for Large z
28.25.1 M ν ( 3 , 4 ) ( z , h ) e ± i ( 2 h cosh z ( 1 2 ν + 1 4 ) π ) ( π h ( cosh z + 1 ) ) 1 2 m = 0 D m ± ( 4 i h ( cosh z + 1 ) ) m ,
The upper signs correspond to M ν ( 3 ) ( z , h ) and the lower signs to M ν ( 4 ) ( z , h ) . The expansion (28.25.1) is valid for M ν ( 3 ) ( z , h ) when …and for M ν ( 4 ) ( z , h ) when …
25: 11.8 Analogs to Kelvin Functions
§11.8 Analogs to Kelvin Functions
26: 11.12 Physical Applications
§11.12 Physical Applications
27: 10.38 Derivatives with Respect to Order
§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 ) ,
For I ν ( z ) / ν at ν = n combine (10.38.1), (10.38.2), and (10.38.4). …
I ν ( z ) ν | ν = 0 = K 0 ( z ) ,
28: 10.27 Connection Formulas
§10.27 Connection Formulas
Other solutions of (10.25.1) are I ν ( z ) and K ν ( z ) .
10.27.1 I n ( z ) = I n ( z ) ,
10.27.3 K ν ( z ) = K ν ( z ) .
Many properties of modified Bessel functions follow immediately from those of ordinary Bessel functions by application of (10.27.6)–(10.27.8).
29: 11.3 Graphics
See accompanying text
Figure 11.3.1: 𝐇 ν ( x ) for 0 x 12 and ν = 0 , 1 2 , 1 , 3 2 , 2 , 3 . Magnify
See accompanying text
Figure 11.3.2: 𝐊 ν ( x ) for 0 < x 16 and ν = 0 , 1 2 , 1 , 3 2 , 2 , 3 . Magnify
See accompanying text
Figure 11.3.3: 𝐇 ν ( x ) for 0 x 12 and ν = 3 , 2 , 3 2 , 1 , 1 2 . Magnify
See accompanying text
Figure 11.3.4: 𝐊 ν ( x ) for 0 < x 16 and ν = 4 , 3 , 2 , 1 , 0 . … Magnify
§11.3(ii) Modified Struve Functions
30: 10.30 Limiting Forms
§10.30(i) z 0
10.30.1 I ν ( z ) ( 1 2 z ) ν / Γ ( ν + 1 ) , ν 1 , 2 , 3 , ,
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).