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11: 28.14 Fourier Series
28.14.1 me ν ( z , q ) = m = c 2 m ν ( q ) e i ( ν + 2 m ) z ,
28.14.4 q c 2 m + 2 ( a ( ν + 2 m ) 2 ) c 2 m + q c 2 m 2 = 0 , a = λ ν ( q ) , c 2 m = c 2 m ν ( q ) ,
28.14.5 m = ( c 2 m ν ( q ) ) 2 = 1 ;
28.14.7 c 2 m ν ( q ) = c 2 m ν ( q ) ,
28.14.8 c 2 m ν ( q ) = ( 1 ) m c 2 m ν ( q ) .
12: 15.7 Continued Fractions
15.7.1 𝐅 ( a , b ; c ; z ) 𝐅 ( a , b + 1 ; c + 1 ; z ) = t 0 u 1 z t 1 u 2 z t 2 u 3 z t 3 ,
13: 31.6 Path-Multiplicative Solutions
14: 31.4 Solutions Analytic at Two Singularities: Heun Functions
For an infinite set of discrete values q m , m = 0 , 1 , 2 , , of the accessory parameter q , the function H ( a , q ; α , β , γ , δ ; z ) is analytic at z = 1 , and hence also throughout the disk | z | < a . … The eigenvalues q m satisfy the continued-fraction equation
31.4.2 q = a γ P 1 Q 1 + q R 1 P 2 Q 2 + q R 2 P 3 Q 3 + q ,
15: 20.16 Software
§20.16(ii) Real Argument and Parameter
§20.16(iii) Complex Argument and/or Parameter
16: 31.2 Differential Equations
All other homogeneous linear differential equations of the second order having four regular singularities in the extended complex plane, { } , can be transformed into (31.2.1). The parameters play different roles: a is the singularity parameter; α , β , γ , δ , ϵ are exponent parameters; q is the accessory parameter. The total number of free parameters is six. … Then (suppressing the parameter k ) … Except for the identity automorphism, each alters the parameters.
17: 8.17 Incomplete Beta Functions
Throughout §§8.17 and 8.18 we assume that a > 0 , b > 0 , and 0 x 1 . …
8.17.4 I x ( a , b ) = 1 I 1 x ( b , a ) .
With a > 0 , b > 0 , and 0 < x < 1 , …
8.17.13 ( a + b ) I x ( a , b ) = a I x ( a + 1 , b ) + b I x ( a , b + 1 ) ,
8.17.16 a I x ( a + 1 , b ) = ( a + c x ) I x ( a , b ) c x I x ( a 1 , b ) ,
18: 9.14 Incomplete Airy Functions
Incomplete Airy functions are defined by the contour integral (9.5.4) when one of the integration limits is replaced by a variable real or complex parameter. …
19: 28.27 Addition Theorems
Addition theorems provide important connections between Mathieu functions with different parameters and in different coordinate systems. …
20: 31.12 Confluent Forms of Heun’s Equation
31.12.1 d 2 w d z 2 + ( γ z + δ z 1 + ϵ ) d w d z + α z q z ( z 1 ) w = 0 .
31.12.2 d 2 w d z 2 + ( δ z 2 + γ z + 1 ) d w d z + α z q z 2 w = 0 .
31.12.3 d 2 w d z 2 ( γ z + δ + z ) d w d z + α z q z w = 0 .
31.12.4 d 2 w d z 2 + ( γ + z ) z d w d z + ( α z q ) w = 0 .