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21: 23.19 Interrelations
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23.19.3 J ⁑ ( Ο„ ) = g 2 3 ⁑ g 2 3 ⁑ 27 ⁒ g 3 2 ⁑ ,
β–Ίwhere g 2 ⁑ , g 3 ⁑ are the invariants of the lattice 𝕃 with generators 1 and Ο„ ; see §23.3(i). …
22: 23.12 Asymptotic Approximations
§23.12 Asymptotic Approximations
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23.12.1 ⁑ ( z ) = Ο€ 2 4 ⁒ Ο‰ 1 2 ⁒ ( 1 3 + csc 2 ⁑ ( Ο€ ⁒ z 2 ⁒ Ο‰ 1 ) + 8 ⁒ ( 1 cos ⁑ ( Ο€ ⁒ z Ο‰ 1 ) ) ⁒ q 2 + O ⁑ ( q 4 ) ) ,
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23.12.2 ΞΆ ⁑ ( z ) = Ο€ 2 4 ⁒ Ο‰ 1 2 ⁒ ( z 3 + 2 ⁒ Ο‰ 1 Ο€ ⁒ cot ⁑ ( Ο€ ⁒ z 2 ⁒ Ο‰ 1 ) 8 ⁒ ( z Ο‰ 1 Ο€ ⁒ sin ⁑ ( Ο€ ⁒ z Ο‰ 1 ) ) ⁒ q 2 + O ⁑ ( q 4 ) ) ,
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23.12.3 Οƒ ⁑ ( z ) = 2 ⁒ Ο‰ 1 Ο€ ⁒ exp ⁑ ( Ο€ 2 ⁒ z 2 24 ⁒ Ο‰ 1 2 ) ⁒ sin ⁑ ( Ο€ ⁒ z 2 ⁒ Ο‰ 1 ) ⁒ ( 1 ( Ο€ 2 ⁒ z 2 Ο‰ 1 2 4 ⁒ sin 2 ⁑ ( Ο€ ⁒ z 2 ⁒ Ο‰ 1 ) ) ⁒ q 2 + O ⁑ ( q 4 ) ) ,
23: 31.2 Differential Equations
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Weierstrass’s Form
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k 2 = ( e 2 ⁑ e 3 ⁑ ) / ( e 1 ⁑ e 3 ⁑ ) ,
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e 1 ⁑ = ⁑ ( Ο‰ 1 ) ,
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e 1 ⁑ + e 2 ⁑ + e 3 ⁑ = 0 ,
β–Ίwhere 2 ⁒ Ο‰ 1 and 2 ⁒ Ο‰ 3 with ⁑ ( Ο‰ 3 / Ο‰ 1 ) > 0 are generators of the lattice 𝕃 for ⁑ ( z | 𝕃 ) . …
24: 27.15 Chinese Remainder Theorem
β–ΊThe Chinese remainder theorem states that a system of congruences x a 1 ( mod m 1 ) , , x a k ( mod m k ) , always has a solution if the moduli are relatively prime in pairs; the solution is unique (mod m ), where m is the product of the moduli. … β–ΊTheir product m has 20 digits, twice the number of digits in the data. …These numbers, in turn, are combined by the Chinese remainder theorem to obtain the final result ( mod m ) , which is correct to 20 digits. …
25: 1.10 Functions of a Complex Variable
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§1.10(ix) Infinite Products
β–ΊThe convergence of the infinite product is uniform if the sequence of partial products converges uniformly. β–Ί
M -test
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Weierstrass Product
26: 20 Theta Functions
Chapter 20 Theta Functions
27: 29.2 Differential Equations
β–Ίwe have β–Ί
29.2.9 d 2 w d η 2 + ( g ν ⁒ ( ν + 1 ) ⁒ ⁑ ( η ) ) ⁒ w = 0 ,
β–Ί β–ΊFor the Weierstrass function see §23.2(ii). …
28: Errata
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  • Subsection 19.25(vi)

    This subsection has been significantly updated. In particular, the following formulae have been corrected. Equation (19.25.35) has been replaced by

    19.25.35 z + 2 ⁒ Ο‰ = ± R F ⁑ ( ⁑ ( z ) e 1 ⁑ , ⁑ ( z ) e 2 ⁑ , ⁑ ( z ) e 3 ⁑ ) ,

    in which the left-hand side z has been replaced by z + 2 ⁒ Ο‰ for some 2 ⁒ Ο‰ 𝕃 , and the right-hand side has been multiplied by ± 1 . Equation (19.25.37) has been replaced by

    19.25.37 ΞΆ ⁑ ( z + 2 ⁒ Ο‰ ) + ( z + 2 ⁒ Ο‰ ) ⁒ ⁑ ( z ) = ± 2 ⁒ R G ⁑ ( ⁑ ( z ) e 1 ⁑ , ⁑ ( z ) e 2 ⁑ , ⁑ ( z ) e 3 ⁑ ) ,

    in which the left-hand side ΞΆ ⁑ ( z ) + z ⁒ ⁑ ( z ) has been replaced by ΞΆ ⁑ ( z + 2 ⁒ Ο‰ ) + ( z + 2 ⁒ Ο‰ ) ⁒ ⁑ ( z ) and the right-hand side has been multiplied by ± 1 . Equation (19.25.39) has been replaced by

    19.25.39 ΞΆ ⁑ ( Ο‰ j ) + Ο‰ j ⁒ e j ⁑ = 2 ⁒ R G ⁑ ( 0 , e j ⁑ e k ⁑ , e j ⁑ e β„“ ⁑ ) ,

    in which the left-hand side Ξ· j was replaced by ΞΆ ⁑ ( Ο‰ j ) , for some 2 ⁒ Ο‰ j 𝕃 and ⁑ ( Ο‰ j ) = e j ⁑ . Equation (19.25.40) has been replaced by

    19.25.40 z + 2 ⁒ Ο‰ = ± Οƒ ⁑ ( z ) ⁒ R F ⁑ ( Οƒ 1 2 ⁒ ( z ) , Οƒ 2 2 ⁒ ( z ) , Οƒ 3 2 ⁒ ( z ) ) ,

    in which the left-hand side z has been replaced by z + 2 ⁒ Ο‰ , and the right-hand side was multiplied by ± 1 . For more details see §19.25(vi).

  • β–Ί
  • Subsection 19.25(vi)

    The Weierstrass lattice roots e j , were linked inadvertently as the base of the natural logarithm. In order to resolve this inconsistency, the lattice roots e j ⁑ , and lattice invariants g 2 ⁑ , g 3 ⁑ , now link to their respective definitions (see §§23.2(i), 23.3(i)).

    Reported by Felix Ospald.

  • β–Ί
  • Equation (19.25.37)

    The Weierstrass zeta function was incorrectly linked to the definition of the Riemann zeta function. However, to the eye, the function appeared correct. The link was corrected.

  • β–Ί
  • Equation (23.2.4)
    23.2.4 ⁑ ( z ) = 1 z 2 + w 𝕃 βˆ– { 0 } ( 1 ( z w ) 2 1 w 2 )

    Originally the denominator ( z w ) 2 was given incorrectly as ( z w 2 ) .

    Reported 2012-02-16 by James D. Walker.

  • β–Ί
  • Chapters 8, 20, 36

    Several new equations have been added. See (8.17.24), (20.7.34), §20.11(v), (26.12.27), (36.2.28), and (36.2.29).

  • 29: 26.12 Plane Partitions
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    26.12.9 ( h = 1 r j = 1 s h + j + t 1 h + j 1 ) 2 ;
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    26.12.10 ( h = 1 r j = 1 s h + j + t 1 h + j 1 ) ⁒ ( h = 1 r + 1 j = 1 s h + j + t 1 h + j 1 ) ;
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    26.12.11 ( h = 1 r + 1 j = 1 s h + j + t 1 h + j 1 ) ⁒ ( h = 1 r j = 1 s + 1 h + j + t 1 h + j 1 ) .
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    26.12.13 h = 1 r j = 1 r h + j + t 1 h + j 1 ;
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    26.12.14 h = 1 r j = 1 r + 1 h + j + t 1 h + j 1 .
    30: Foreword
    β–ΊThe production of these new resources has been a very complex undertaking some 10 years in the making. … β–ΊNovember 20, 2009 …