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21: 36.9 Integral Identities
For these results and also integrals over doubly-infinite intervals see Berry and Wright (1980). …
22: 1.15 Summability Methods
§1.15 Summability Methods
§1.15(vi) Fractional Integrals
23: 19.3 Graphics
See accompanying text
Figure 19.3.3: F ( ϕ , k ) as a function of k 2 and sin 2 ϕ for 1 k 2 2 , 0 sin 2 ϕ 1 . If sin 2 ϕ = 1 ( k 2 ), then the function reduces to K ( k ) , becoming infinite when k 2 = 1 . … Magnify 3D Help
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Figure 19.3.9: ( K ( k ) ) as a function of complex k 2 for 2 ( k 2 ) 2 , 2 ( k 2 ) 2 . …On the branch cut ( k 2 1 ) it is infinite at k 2 = 1 , and has the value K ( 1 / k ) / k when k 2 > 1 . Magnify 3D Help
24: 25.12 Polylogarithms
25.12.9 n = 1 sin ( n θ ) n 2 = 0 θ ln ( 2 sin ( 1 2 x ) ) d x .
25: 27.12 Asymptotic Formulas: Primes
π ( x ) li ( x ) changes sign infinitely often as x ; see Littlewood (1914), Bays and Hudson (2000). …
26: 19.5 Maclaurin and Related Expansions
An infinite series for ln K ( k ) is equivalent to the infinite product …
27: 13.16 Integral Representations
13.16.2 M κ , μ ( z ) = Γ ( 1 + 2 μ ) z λ Γ ( 1 + 2 μ 2 λ ) Γ ( 2 λ ) 0 1 M κ λ , μ λ ( z t ) e 1 2 z ( t 1 ) t μ λ 1 2 ( 1 t ) 2 λ 1 d t , μ + 1 2 > λ > 0 ,
28: 5.17 Barnes’ G -Function (Double Gamma Function)
5.17.2 G ( n ) = ( n 2 ) ! ( n 3 ) ! 1 ! , n = 2 , 3 , .
5.17.3 G ( z + 1 ) = ( 2 π ) z / 2 exp ( 1 2 z ( z + 1 ) 1 2 γ z 2 ) k = 1 ( ( 1 + z k ) k exp ( z + z 2 2 k ) ) .
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 .
29: 7.13 Zeros
In the first quadrant of C ( z ) has an infinite set of zeros z n = x n + i y n , n = 1 , 2 , 3 , , arranged in order of increasing absolute value. …
30: 3.5 Quadrature
For computing infinite oscillatory integrals, Longman’s method may be used. …