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31: 20.10 Integrals
20.10.1 0 x s 1 θ 2 ( 0 | i x 2 ) d x = 2 s ( 1 2 s ) π s / 2 Γ ( 1 2 s ) ζ ( s ) , s > 1 ,
20.10.2 0 x s 1 ( θ 3 ( 0 | i x 2 ) 1 ) d x = π s / 2 Γ ( 1 2 s ) ζ ( s ) , s > 1 ,
20.10.3 0 x s 1 ( 1 θ 4 ( 0 | i x 2 ) ) d x = ( 1 2 1 s ) π s / 2 Γ ( 1 2 s ) ζ ( s ) , s > 0 .
Let s , , and β be constants such that s > 0 , > 0 , and | β | + | β | . …
32: 20.1 Special Notation
m , n integers.
q ( ) the nome, q = e i π τ , 0 < | q | < 1 . Since τ is not a single-valued function of q , it is assumed that τ is known, even when q is specified. Most applications concern the rectangular case τ = 0 , τ > 0 , so that 0 < q < 1 and τ and q are uniquely related.
33: 21.1 Special Notation
g , h positive integers.
g × × × ( g times).
𝛀 g × g complex, symmetric matrix with 𝛀 strictly positive definite, i.e., a Riemann matrix.
Lowercase boldface letters or numbers are g -dimensional real or complex vectors, either row or column depending on the context. Uppercase boldface letters are g × g real or complex matrices. … The function Θ ( ϕ | 𝐁 ) = θ ( ϕ / ( 2 π i ) | 𝐁 / ( 2 π i ) ) is also commonly used; see, for example, Belokolos et al. (1994, §2.5), Dubrovin (1981), and Fay (1973, Chapter 1).
34: 28.20 Definitions and Basic Properties
as z + with π + δ z 2 π δ , and …as z + with 2 π + δ z π δ . …as z + with | z | π δ . …
35: 32.11 Asymptotic Approximations for Real Variables
32.11.21 σ = sign ( s ) ,
32.11.22 ρ 2 = π 1 ln ( ( 1 + | s | 2 ) / | 2 s | ) ,
36: 6.7 Integral Representations
6.7.7 0 1 e a t sin ( b t ) t d t = Ein ( a + i b ) , a , b ,
6.7.8 0 1 e a t ( 1 cos ( b t ) ) t d t = Ein ( a + i b ) Ein ( a ) , a , b .
6.7.11 0 1 ( 1 e a t ) cos ( b t ) t d t = Ein ( a + i b ) Cin ( b ) , a , b .
37: 7.7 Integral Representations
7.7.3 0 e a t 2 + 2 i z t d t = 1 2 π a e z 2 / a + i a F ( z a ) , a > 0 .
38: 4.38 Inverse Hyperbolic Functions: Further Properties
4.38.6 arctanh z = ± i π 2 + 1 z + 1 3 z 3 + 1 5 z 5 + , z 0 , | z | 1 .
4.38.7 arctanh z = z 1 z 2 ( 1 + 2 3 z 2 z 2 1 + 2 4 3 5 ( z 2 z 2 1 ) 2 + ) , ( z 2 ) < 1 2 ,
which requires z ( = x + i y ) to lie between the two rectangular hyperbolas given by …
4.38.10 d d z arccosh z = ± ( z 2 1 ) 1 / 2 , z 0 .
4.38.12 d d z arccsch z = 1 z ( 1 + z 2 ) 1 / 2 , z 0 .
39: 33.22 Particle Scattering and Atomic and Molecular Spectra
At negative energies E < 0 and both ρ and η are purely imaginary. …
i 𝗄 Scaling
The i 𝗄 -scaled variables z and κ of §13.2 are given by …
  • Searches for resonances as poles of the S -matrix in the complex half-plane 𝗄 < 𝟢 . See for example Csótó and Hale (1997).

  • Eigenstates using complex-rotated coordinates r r e i θ , so that resonances have square-integrable eigenfunctions. See for example Halley et al. (1993).

  • 40: 25.6 Integer Arguments
    25.6.7 ζ ( 2 ) = 0 1 0 1 1 1 x y d x d y .
    25.6.13 ( 1 ) k ζ ( k ) ( 2 n ) = 2 ( 1 ) n ( 2 π ) 2 n + 1 m = 0 k r = 0 m ( k m ) ( m r ) ( c k m ) Γ ( r ) ( 2 n + 1 ) ζ ( m r ) ( 2 n + 1 ) ,
    25.6.14 ( 1 ) k ζ ( k ) ( 1 2 n ) = 2 ( 1 ) n ( 2 π ) 2 n m = 0 k r = 0 m ( k m ) ( m r ) ( c k m ) Γ ( r ) ( 2 n ) ζ ( m r ) ( 2 n ) ,