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11: 23.22 Methods of Computation
  • (a)

    In the general case, given by c d 0 , we compute the roots α , β , γ , say, of the cubic equation 4 t 3 c t d = 0 ; see §1.11(iii). These roots are necessarily distinct and represent e 1 , e 2 , e 3 in some order.

    If c and d are real, and the discriminant is positive, that is c 3 27 d 2 > 0 , then e 1 , e 2 , e 3 can be identified via (23.5.1), and k 2 , k 2 obtained from (23.6.16).

    If c 3 27 d 2 < 0 , or c and d are not both real, then we label α , β , γ so that the triangle with vertices α , β , γ is positively oriented and [ α , γ ] is its longest side (chosen arbitrarily if there is more than one). In particular, if α , β , γ are collinear, then we label them so that β is on the line segment ( α , γ ) . In consequence, k 2 = ( β γ ) / ( α γ ) , k 2 = ( α β ) / ( α γ ) satisfy k 2 0 k 2 (with strict inequality unless α , β , γ are collinear); also | k 2 | , | k 2 | 1 .

    Finally, on taking the principal square roots of k 2 and k 2 we obtain values for k and k that lie in the 1st and 4th quadrants, respectively, and 2 ω 1 , 2 ω 3 are given by

    23.22.1 2 ω 1 M ( 1 , k ) = 2 i ω 3 M ( 1 , k ) = π 3 c ( 2 + k 2 k 2 ) ( k 2 k 2 ) d ( 1 k 2 k 2 ) ,

    where M denotes the arithmetic-geometric mean (see §§19.8(i) and 22.20(ii)). This process yields 2 possible pairs ( 2 ω 1 , 2 ω 3 ), corresponding to the 2 possible choices of the square root.

  • 12: DLMF Project News
    error generating summary
    13: 5.2 Definitions
    5.2.5 ( a ) n = Γ ( a + n ) / Γ ( a ) , a 0 , 1 , 2 , .
    5.2.6 ( a ) n = ( 1 ) n ( a n + 1 ) n ,
    5.2.7 ( m ) n = { ( 1 ) n m ! ( m n ) ! , 0 n m , 0 , n > m ,
    14: 6.1 Special Notation
    The main functions treated in this chapter are the exponential integrals Ei ( x ) , E 1 ( z ) , and Ein ( z ) ; the logarithmic integral li ( x ) ; the sine integrals Si ( z ) and si ( z ) ; the cosine integrals Ci ( z ) and Cin ( z ) . …
    15: 28.8 Asymptotic Expansions for Large q
    They are derived by rigorous analysis and accompanied by strict and realistic error bounds. …
    16: 17.2 Calculus
    For n = 0 , 1 , 2 , ,
    17.2.1 ( a ; q ) n = ( 1 a ) ( 1 a q ) ( 1 a q n 1 ) ,
    17.2.3 ( a ; q ) ν = j = 0 ( 1 a q j 1 a q ν + j ) ,
    17.2.4 ( a ; q ) = j = 0 ( 1 a q j ) ,
    17.2.7 ( a ; q 1 ) n = ( a 1 ; q ) n ( a ) n q ( n 2 ) ,
    17: 33.2 Definitions and Basic Properties
    33.2.9 θ ( η , ρ ) = ρ η ln ( 2 ρ ) 1 2 π + σ ( η ) ,
    33.2.10 σ ( η ) = ph Γ ( + 1 + i η ) ,
    σ ( η ) is the Coulomb phase shift. … Also, e i σ ( η ) H ± ( η , ρ ) are analytic functions of η when < η < . …
    18: 17.5 ϕ 0 0 , ϕ 0 1 , ϕ 1 1 Functions
    17.5.1 ϕ 0 0 ( ; ; q , z ) = n = 0 ( 1 ) n q ( n 2 ) z n ( q ; q ) n = ( z ; q ) ;
    17.5.5 ϕ 1 1 ( a c ; q , c / a ) = ( c / a ; q ) ( c ; q ) .
    19: 17.3 q -Elementary and q -Special Functions
    17.3.1 e q ( x ) = n = 0 ( 1 q ) n x n ( q ; q ) n = 1 ( ( 1 q ) x ; q ) ,
    17.3.2 E q ( x ) = n = 0 ( 1 q ) n q ( n 2 ) x n ( q ; q ) n = ( ( 1 q ) x ; q ) .
    17.3.3 sin q ( x ) = 1 2 i ( e q ( i x ) e q ( i x ) ) = n = 0 ( 1 q ) 2 n + 1 ( 1 ) n x 2 n + 1 ( q ; q ) 2 n + 1 ,
    17.3.4 Sin q ( x ) = 1 2 i ( E q ( i x ) E q ( i x ) ) = n = 0 ( 1 q ) 2 n + 1 q n ( 2 n + 1 ) ( 1 ) n x 2 n + 1 ( q ; q ) 2 n + 1 .
    17.3.5 cos q ( x ) = 1 2 ( e q ( i x ) + e q ( i x ) ) = n = 0 ( 1 q ) 2 n ( 1 ) n x 2 n ( q ; q ) 2 n ,
    20: 18.7 Interrelations and Limit Relations
    18.7.1 C n ( λ ) ( x ) = ( 2 λ ) n ( λ + 1 2 ) n P n ( λ 1 2 , λ 1 2 ) ( x ) ,
    18.7.2 P n ( α , α ) ( x ) = ( α + 1 ) n ( 2 α + 1 ) n C n ( α + 1 2 ) ( x ) .
    18.7.7 T n ( x ) = T n ( 2 x 1 ) ,
    18.7.8 U n ( x ) = U n ( 2 x 1 ) .
    18.7.10 P n ( x ) = P n ( 2 x 1 ) .