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1: 23.19 Interrelations
23.19.2 J ( τ ) = 4 27 ( 1 λ ( τ ) + λ 2 ( τ ) ) 3 ( λ ( τ ) ( 1 λ ( τ ) ) ) 2 ,
23.19.3 J ( τ ) = g 2 3 g 2 3 27 g 3 2 ,
where g 2 , g 3 are the invariants of the lattice 𝕃 with generators 1 and τ ; see §23.3(i). …
2: 23.16 Graphics
See Figures 23.16.123.16.3 for the modular functions λ , J , and η . …
See accompanying text
Figure 23.16.1: Modular functions λ ( i y ) , J ( i y ) , η ( i y ) for 0 y 3 . … Magnify
3: 23.17 Elementary Properties
J ( i ) = 1 ,
J ( e π i / 3 ) = 0 ,
For further results for J ( τ ) see Cohen (1993, p. 376). …
23.17.5 1728 J ( τ ) = q 2 + 744 + 1 96884 q 2 + 214 93760 q 4 + ,
4: 23.18 Modular Transformations
Klein’s Complete Invariant
23.18.4 J ( 𝒜 τ ) = J ( τ ) .
J ( τ ) is a modular form of level zero for SL ( 2 , ) . …
5: 23.15 Definitions
§23.15(ii) Functions λ ( τ ) , J ( τ ) , η ( τ )
Klein’s Complete Invariant
23.15.7 J ( τ ) = ( θ 2 8 ( 0 , q ) + θ 3 8 ( 0 , q ) + θ 4 8 ( 0 , q ) ) 3 54 ( θ 1 ( 0 , q ) ) 8 ,
6: 23.1 Special Notation
𝕃 lattice in .
K ( k ) , K ( k ) complete elliptic integrals (§19.2(i)).
Δ discriminant g 2 3 27 g 3 2 .
The main functions treated in this chapter are the Weierstrass -function ( z ) = ( z | 𝕃 ) = ( z ; g 2 , g 3 ) ; the Weierstrass zeta function ζ ( z ) = ζ ( z | 𝕃 ) = ζ ( z ; g 2 , g 3 ) ; the Weierstrass sigma function σ ( z ) = σ ( z | 𝕃 ) = σ ( z ; g 2 , g 3 ) ; the elliptic modular function λ ( τ ) ; Klein’s complete invariant J ( τ ) ; Dedekind’s eta function η ( τ ) . …
7: 20 Theta Functions
Chapter 20 Theta Functions
8: Bibliography B
  • G. Backenstoss (1970) Pionic atoms. Annual Review of Nuclear and Particle Science 20, pp. 467–508.
  • A. R. Barnett (1981b) KLEIN: Coulomb functions for real λ and positive energy to high accuracy. Comput. Phys. Comm. 24 (2), pp. 141–159.
  • K. L. Bell and N. S. Scott (1980) Coulomb functions (negative energies). Comput. Phys. Comm. 20 (3), pp. 447–458.
  • W. G. Bickley (1935) Some solutions of the problem of forced convection. Philos. Mag. Series 7 20, pp. 322–343.
  • P. Boalch (2005) From Klein to Painlevé via Fourier, Laplace and Jimbo. Proc. London Math. Soc. (3) 90 (1), pp. 167–208.
  • 9: 15.17 Mathematical Applications
    §15.17(ii) Conformal Mappings
    See Klein (1894) and Hochstadt (1971). Hypergeometric functions, especially complete elliptic integrals, also play an important role in quasiconformal mapping. …
    10: Gergő Nemes
    As of September 20, 2021, Nemes performed a complete analysis and acted as main consultant for the update of the source citation and proof metadata for every formula in Chapter 25 Zeta and Related Functions. …