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F-homotopic transformations

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21: 6.14 Integrals
§6.14(i) Laplace Transforms
22: 23.18 Modular Transformations
§23.18 Modular Transformations
23.18.3 λ ( 𝒜 τ ) = λ ( τ ) ,
23.18.4 J ( 𝒜 τ ) = J ( τ ) .
23.18.5 η ( 𝒜 τ ) = ε ( 𝒜 ) ( i ( c τ + d ) ) 1 / 2 η ( τ ) ,
23.18.6 ε ( 𝒜 ) = exp ( π i ( a + d 12 c + s ( d , c ) ) ) ,
23: Mark J. Ablowitz
for appropriate data they can be linearized by the Inverse Scattering Transform (IST) and they possess solitons as special solutions. …Some of the relationships between IST and Painlevé equations are discussed in two books: Solitons and the Inverse Scattering Transform and Solitons, Nonlinear Evolution Equations and Inverse Scattering. …
24: 13.23 Integrals
§13.23(i) Laplace and Mellin Transforms
§13.23(ii) Fourier Transforms
§13.23(iii) Hankel Transforms
§13.23(iv) Integral Transforms in terms of Whittaker Functions
25: 22.17 Moduli Outside the Interval [0,1]
§22.17(ii) Complex Moduli
In particular, the Landen transformations in §§22.7(i) and 22.7(ii) are valid for all complex values of k , irrespective of which values of k and k = 1 k 2 are chosen—as long as they are used consistently. …
26: 13.10 Integrals
§13.10(ii) Laplace Transforms
§13.10(iii) Mellin Transforms
§13.10(iv) Fourier Transforms
§13.10(v) Hankel Transforms
27: 10.74 Methods of Computation
Hankel Transform
Spherical Bessel Transform
The spherical Bessel transform is the Hankel transform (10.22.76) in the case when ν is half an odd positive integer. …
Kontorovich–Lebedev Transform
28: 21.5 Modular Transformations
§21.5 Modular Transformations
§21.5(i) Riemann Theta Functions
Equation (21.5.4) is the modular transformation property for Riemann theta functions. …
§21.5(ii) Riemann Theta Functions with Characteristics
For explicit results in the case g = 1 , see §20.7(viii).
29: 15.19 Methods of Computation
For z it is always possible to apply one of the linear transformations in §15.8(i) in such a way that the hypergeometric function is expressed in terms of hypergeometric functions with an argument in the interval [ 0 , 1 2 ] . For z it is possible to use the linear transformations in such a way that the new arguments lie within the unit circle, except when z = e ± π i / 3 . This is because the linear transformations map the pair { e π i / 3 , e π i / 3 } onto itself. … When z > 1 2 it is better to begin with one of the linear transformations (15.8.4), (15.8.7), or (15.8.8). … …
30: Bibliography W
  • G. N. Watson (1910) The cubic transformation of the hypergeometric function. Quart. J. Pure and Applied Math. 41, pp. 70–79.
  • F. J. W. Whipple (1927) Some transformations of generalized hypergeometric series. Proc. London Math. Soc. (2) 26 (2), pp. 257–272.
  • D. V. Widder (1979) The Airy transform. Amer. Math. Monthly 86 (4), pp. 271–277.
  • D. V. Widder (1941) The Laplace Transform. Princeton Mathematical Series, v. 6, Princeton University Press, Princeton, NJ.
  • J. Wimp (1964) A class of integral transforms. Proc. Edinburgh Math. Soc. (2) 14, pp. 33–40.