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11: 17.18 Methods of Computation
For computation of the q -exponential function see Gabutti and Allasia (2008). …
12: 8.5 Confluent Hypergeometric Representations
8.5.1 γ ( a , z ) = a - 1 z a e - z M ( 1 , 1 + a , z ) = a - 1 z a M ( a , 1 + a , - z ) , a 0 , - 1 , - 2 , .
8.5.2 γ * ( a , z ) = e - z M ( 1 , 1 + a , z ) = M ( a , 1 + a , - z ) .
8.5.3 Γ ( a , z ) = e - z U ( 1 - a , 1 - a , z ) = z a e - z U ( 1 , 1 + a , z ) .
8.5.4 γ ( a , z ) = a - 1 z 1 2 a - 1 2 e - 1 2 z M 1 2 a - 1 2 , 1 2 a ( z ) .
8.5.5 Γ ( a , z ) = e - 1 2 z z 1 2 a - 1 2 W 1 2 a - 1 2 , 1 2 a ( z ) .
13: 9.5 Integral Representations
9.5.3 Bi ( x ) = 1 π 0 exp ( - 1 3 t 3 + x t ) d t + 1 π 0 sin ( 1 3 t 3 + x t ) d t .
9.5.4 Ai ( z ) = 1 2 π i e - π i / 3 e π i / 3 exp ( 1 3 t 3 - z t ) d t ,
9.5.5 Bi ( z ) = 1 2 π - e π i / 3 exp ( 1 3 t 3 - z t ) d t + 1 2 π - e - π i / 3 exp ( 1 3 t 3 - z t ) d t .
9.5.6 Ai ( z ) = 3 2 π 0 exp ( - t 3 3 - z 3 3 t 3 ) d t , | ph z | < 1 6 π .
9.5.7 Ai ( z ) = e - ζ π 0 exp ( - z 1 / 2 t 2 ) cos ( 1 3 t 3 ) d t , | ph z | < π .
14: 18.32 OP’s with Respect to Freud Weights
18.32.1 w ( x ) = exp ( - Q ( x ) ) , - < x < ,
15: 36.11 Leading-Order Asymptotics
36.11.3 Ψ 2 ( 0 , y ) = { π / y ( exp ( 1 4 i π ) + o ( 1 ) ) , y + , π / | y | exp ( - 1 4 i π ) ( 1 + i 2 exp ( - 1 4 i y 2 ) + o ( 1 ) ) , y - .
36.11.4 Ψ 3 ( x , 0 , 0 ) = 2 π ( 5 | x | 3 ) 1 / 8 { exp ( - 2 2 ( x / 5 ) 5 / 4 ) ( cos ( 2 2 ( x / 5 ) 5 / 4 - 1 8 π ) + o ( 1 ) ) , x + , cos ( 4 ( | x | / 5 ) 5 / 4 - 1 4 π ) + o ( 1 ) , x - .
36.11.5 Ψ 3 ( 0 , y , 0 ) = Ψ 3 ( 0 , - y , 0 ) ¯ = exp ( 1 4 i π ) π / y ( 1 - ( i / 3 ) exp ( 3 2 i ( 2 y / 5 ) 5 / 3 ) + o ( 1 ) ) , y + .
36.11.7 Ψ ( E ) ( 0 , 0 , z ) = π z ( i + 3 exp ( 4 27 i z 3 ) + o ( 1 ) ) , z ± ,
36.11.8 Ψ ( H ) ( 0 , 0 , z ) = 2 π z ( 1 - i 3 exp ( 1 27 i z 3 ) + o ( 1 ) ) , z ± .
16: 7.9 Continued Fractions
7.9.1 π e z 2 erfc z = z z 2 + 1 2 1 + 1 z 2 + 3 2 1 + 2 z 2 + , z > 0 ,
7.9.2 π e z 2 erfc z = 2 z 2 z 2 + 1 - 1 2 2 z 2 + 5 - 3 4 2 z 2 + 9 - , z > 0 ,
17: 4.7 Derivatives and Differential Equations
§4.7(ii) Exponentials and Powers
The general solution of the differential equation …
4.7.13 w = exp ( f ( z ) d z ) + constant .
18: 20.8 Watson’s Expansions
20.8.1 θ 2 ( 0 , q ) θ 3 ( z , q ) θ 4 ( z , q ) θ 2 ( z , q ) = 2 n = - ( - 1 ) n q n 2 e i 2 n z q - n e - i z + q n e i z .
19: 13.27 Mathematical Applications
Vilenkin (1968, Chapter 8) constructs irreducible representations of this group, in which the diagonal matrices correspond to operators of multiplication by an exponential function. …
20: 4.14 Definitions and Periodicity
4.14.1 sin z = e i z - e - i z 2 i ,
4.14.2 cos z = e i z + e - i z 2 ,
4.14.3 cos z ± i sin z = e ± i z ,