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31: 8.4 Special Values
8.4.13 Γ ( 1 n , z ) = z 1 n E n ( z ) ,
32: 13.6 Relations to Other Functions
When a b is an integer or a is a positive integer the Kummer functions can be expressed as incomplete gamma functions (or generalized exponential integrals). …
13.6.6 U ( a , a , z ) = z 1 a U ( 1 , 2 a , z ) = z 1 a e z E a ( z ) = e z Γ ( 1 a , z ) .
33: Bibliography
  • Z. Altaç (1996) Integrals involving Bickley and Bessel functions in radiative transfer, and generalized exponential integral functions. J. Heat Transfer 118 (3), pp. 789–792.
  • G. D. Anderson, S.-L. Qiu, M. K. Vamanamurthy, and M. Vuorinen (2000) Generalized elliptic integrals and modular equations. Pacific J. Math. 192 (1), pp. 1–37.
  • 34: Bibliography C
  • L. G. Cabral-Rosetti and M. A. Sanchis-Lozano (2000) Generalized hypergeometric functions and the evaluation of scalar one-loop integrals in Feynman diagrams. J. Comput. Appl. Math. 115 (1-2), pp. 93–99.
  • B. C. Carlson (1999) Toward symbolic integration of elliptic integrals. J. Symbolic Comput. 28 (6), pp. 739–753.
  • C. Chiccoli, S. Lorenzutta, and G. Maino (1987) A numerical method for generalized exponential integrals. Comput. Math. Appl. 14 (4), pp. 261–268.
  • C. Chiccoli, S. Lorenzutta, and G. Maino (1988) On the evaluation of generalized exponential integrals E v ( x ) . J. Comput. Phys. 78 (2), pp. 278–287.
  • C. Chiccoli, S. Lorenzutta, and G. Maino (1990b) On a Tricomi series representation for the generalized exponential integral. Internat. J. Comput. Math. 31, pp. 257–262.
  • 35: 2.3 Integrals of a Real Variable
    (In other words, differentiation of (2.3.8) with respect to the parameter λ (or μ ) is legitimate.) … For the more general integral (2.3.19) we assume, without loss of generality, that the stationary point (if any) is at the left endpoint. … For extensions to oscillatory integrals with more general t -powers and logarithmic singularities see Wong and Lin (1978) and Sidi (2010). …
    36: 5.17 Barnes’ G -Function (Double Gamma Function)
    5.17.4 Ln G ( z + 1 ) = 1 2 z ln ( 2 π ) 1 2 z ( z + 1 ) + z Ln Γ ( z + 1 ) 0 z Ln Γ ( t + 1 ) d t .
    37: 13.23 Integrals
    13.23.4 0 e z t t ν 1 W κ , μ ( t ) d t = Γ ( 1 2 + μ + ν ) Γ ( 1 2 μ + ν ) 𝐅 1 2 ( 1 2 μ + ν , 1 2 + μ + ν ν κ + 1 ; 1 2 z ) , ( ν + 1 2 ) > | μ | , z > 1 2 ,
    Generalized orthogonality integrals (33.14.13) and (33.14.15) can be expressed in terms of Whittaker functions via the definitions in that section.
    38: 6.2 Definitions and Interrelations
    The generalized exponential integral E p ( z ) , p , is treated in Chapter 8. …
    39: 5.9 Integral Representations
    5.9.10 Ln Γ ( z ) = ( z 1 2 ) ln z z + 1 2 ln ( 2 π ) + 2 0 arctan ( t / z ) e 2 π t 1 d t ,
    5.9.10_1 Ln Γ ( z ) = ( z 1 2 ) ln z z + 1 2 ln ( 2 π ) z π 0 ln ( 1 e 2 π t ) t 2 + z 2 d t ,
    5.9.10_2 Ln Γ ( z ) = ( z 1 2 ) ln z z + 1 2 ln ( 2 π ) + 0 e z t ( 1 e t 1 1 t + 1 2 ) d t t ,
    5.9.11 Ln Γ ( z + 1 ) = γ z 1 2 π i c i c + i π z s s sin ( π s ) ζ ( s ) d s ,
    40: Bibliography M
  • P. Midy (1975) An improved calculation of the general elliptic integral of the second kind in the neighbourhood of x = 0 . Numer. Math. 25 (1), pp. 99–101.
  • G. F. Miller (1960) Tables of Generalized Exponential Integrals. NPL Mathematical Tables, Vol. III, Her Majesty’s Stationery Office, London.