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11: 13.4 Integral Representations
where the contour of integration separates the poles of Γ ( a + t ) from those of Γ ( t ) . … where the contour of integration separates the poles of Γ ( a + t ) Γ ( 1 + a b + t ) from those of Γ ( t ) . …
12: 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 ) . …
13: 28.33 Physical Applications
where q = 1 4 c 2 k 2 and a n ( q ) or b n ( q ) is the separation constant; compare (28.12.11), (28.20.11), and (28.20.12). …
14: 10.32 Integral Representations
In (10.32.14) the integration contour separates the poles of Γ ( t ) from the poles of Γ ( 1 2 t ν ) Γ ( 1 2 t + ν ) . …
15: 16.17 Definition
where the integration path L separates the poles of the factors Γ ( b s ) from those of the factors Γ ( 1 a + s ) . …
16: 9.12 Scorer Functions
where the integration contour separates the poles of Γ ( 1 3 + 1 3 t ) from those of Γ ( t ) . …
17: Bibliography K
  • E. G. Kalnins (1986) Separation of Variables for Riemannian Spaces of Constant Curvature. Longman Scientific & Technical, Harlow.
  • 18: 10.9 Integral Representations
    where the path of integration separates the poles of Γ ( t ) from those of Γ ( 2 t + μ + ν + 1 ) . …
    19: Bibliography O
  • M. N. Olevskiĭ (1950) Triorthogonal systems in spaces of constant curvature in which the equation Δ 2 u + λ u = 0 allows a complete separation of variables. Mat. Sbornik N.S. 27(69) (3), pp. 379–426 (Russian).
  • 20: 8.6 Integral Representations
    In (8.6.10)–(8.6.12), c is a real constant and the path of integration is indented (if necessary) so that in the case of (8.6.10) it separates the poles of the gamma function from the pole at s = a , in the case of (8.6.11) it is to the right of all poles, and in the case of (8.6.12) it separates the poles of the gamma function from the poles at s = 0 , 1 , 2 , . …