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21: 16.5 Integral Representations and Integrals
§16.5 Integral Representations and Integrals
where the contour of integration separates the poles of Γ ( a k + s ) , k = 1 , , p , from those of Γ ( s ) . …
22: 33.2 Definitions and Basic Properties
§33.2(i) Coulomb Wave Equation
§33.2(ii) Regular Solution F ( η , ρ )
F ( η , ρ ) is a real and analytic function of ρ on the open interval 0 < ρ < , and also an analytic function of η when < η < . … As in the case of F ( η , ρ ) , the solutions H ± ( η , ρ ) and G ( η , ρ ) are analytic functions of ρ when 0 < ρ < . Also, e i σ ( η ) H ± ( η , ρ ) are analytic functions of η when < η < . …
23: 16.15 Integral Representations and Integrals
These representations can be used to derive analytic continuations of the Appell functions, including convergent series expansions for large x , large y , or both. …
24: 35.2 Laplace Transform
where the integration variable 𝐗 ranges over the space 𝛀 . … Then (35.2.1) converges absolutely on the region ( 𝐙 ) > 𝐗 0 , and g ( 𝐙 ) is a complex analytic function of all elements z j , k of 𝐙 . …
25: 23.15 Definitions
If, as a function of q , f ( τ ) is analytic at q = 0 , then f ( τ ) is called a modular form. … …
26: 25.15 Dirichlet L -functions
§25.15(i) Definitions and Basic Properties
For the principal character χ 1 ( mod k ) , L ( s , χ 1 ) is analytic everywhere except for a simple pole at s = 1 with residue ϕ ( k ) / k , where ϕ ( k ) is Euler’s totient function27.2). …
27: 21.2 Definitions
21.2.1 θ ( 𝐳 | 𝛀 ) = 𝐧 g e 2 π i ( 1 2 𝐧 𝛀 𝐧 + 𝐧 𝐳 ) .
This g -tuple Fourier series converges absolutely and uniformly on compact sets of the 𝐳 and 𝛀 spaces; hence θ ( 𝐳 | 𝛀 ) is an analytic function of (each element of) 𝐳 and (each element of) 𝛀 . …
28: 28.12 Definitions and Basic Properties
If q is a normal value of the corresponding equation (28.2.16), then these functions are uniquely determined as analytic functions of z and q by the normalization …
§28.12(iii) Functions ce ν ( z , q ) , se ν ( z , q ) , when ν
29: 33.14 Definitions and Basic Properties
§33.14(i) Coulomb Wave Equation
§33.14(ii) Regular Solution f ( ϵ , ; r )
f ( ϵ , ; r ) is real and an analytic function of r in the interval < r < , and it is also an analytic function of ϵ when < ϵ < . …
§33.14(iii) Irregular Solution h ( ϵ , ; r )
h ( ϵ , ; r ) is real and an analytic function of each of r and ϵ in the intervals < r < and < ϵ < , except when r = 0 or ϵ = 0 . …
30: 2.10 Sums and Sequences
Let f ( z ) be analytic on the annulus 0 < | z | < r , with Laurent expansion
2.10.25 f ( z ) = n = f n z n , 0 < | z | < r .
  • (b´)

    On the circle | z | = r , the function f ( z ) g ( z ) has a finite number of singularities, and at each singularity z j , say,

    2.10.30 f ( z ) g ( z ) = O ( ( z z j ) σ j 1 ) , z z j ,

    where σ j is a positive constant.

  • 2.10.32 f ( m ) ( z ) g ( m ) ( z ) = O ( ( z z j ) σ j 1 ) ,