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21: 4.7 Derivatives and Differential Equations
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4.7.2 d d z ⁑ Ln ⁑ z = 1 z ,
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4.7.4 d n d z n ⁑ Ln ⁑ z = ( 1 ) n 1 ⁒ ( n 1 ) ! ⁒ z n .
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4.7.6 w ⁑ ( z ) = Ln ⁑ ( f ⁑ ( z ) ) +  constant .
22: 5.10 Continued Fractions
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5.10.1 Ln ⁑ Ξ“ ⁑ ( z ) + z ( z 1 2 ) ⁒ ln ⁑ z 1 2 ⁒ ln ⁑ ( 2 ⁒ Ο€ ) = a 0 z + a 1 z + a 2 z + a 3 z + a 4 z + a 5 z + ⁒ β‹― ,
23: 5.17 Barnes’ G -Function (Double Gamma Function)
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5.17.4 Ln ⁑ G ⁑ ( z + 1 ) = 1 2 ⁒ z ⁒ ln ⁑ ( 2 ⁒ Ο€ ) 1 2 ⁒ z ⁒ ( z + 1 ) + z ⁒ Ln ⁑ Ξ“ ⁑ ( z + 1 ) 0 z Ln ⁑ Ξ“ ⁑ ( t + 1 ) ⁒ d t .
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5.17.5 Ln ⁑ G ⁑ ( z + 1 ) 1 4 ⁒ z 2 + z ⁒ Ln ⁑ Ξ“ ⁑ ( z + 1 ) ( 1 2 ⁒ z ⁒ ( z + 1 ) + 1 12 ) ⁒ ln ⁑ z ln ⁑ A + k = 1 B 2 ⁒ k + 2 2 ⁒ k ⁒ ( 2 ⁒ k + 1 ) ⁒ ( 2 ⁒ k + 2 ) ⁒ z 2 ⁒ k .
24: 22.15 Inverse Functions
β–ΊEach of these inverse functions is multivalued. …
25: 22.14 Integrals
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22.14.2 cn ⁑ ( x , k ) ⁒ d x = k 1 ⁒ Arccos ⁑ ( dn ⁑ ( x , k ) ) ,
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22.14.3 dn ⁑ ( x , k ) ⁒ d x = Arcsin ⁑ ( sn ⁑ ( x , k ) ) = am ⁑ ( x , k ) .
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22.14.5 sd ⁑ ( x , k ) ⁒ d x = ( k ⁒ k ) 1 ⁒ Arcsin ⁑ ( k ⁒ cd ⁑ ( x , k ) ) ,
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22.14.6 nd ⁑ ( x , k ) ⁒ d x = k 1 ⁒ Arccos ⁑ ( cd ⁑ ( x , k ) ) .
26: 6.4 Analytic Continuation
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6.4.1 E 1 ⁑ ( z ) = Ein ⁑ ( z ) Ln ⁑ z γ ;
27: 5.11 Asymptotic Expansions
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5.11.1 Ln ⁑ Ξ“ ⁑ ( z ) ( z 1 2 ) ⁒ ln ⁑ z z + 1 2 ⁒ ln ⁑ ( 2 ⁒ Ο€ ) + k = 1 B 2 ⁒ k 2 ⁒ k ⁒ ( 2 ⁒ k 1 ) ⁒ z 2 ⁒ k 1
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5.11.8 Ln ⁑ Ξ“ ⁑ ( z + h ) ( z + h 1 2 ) ⁒ ln ⁑ z z + 1 2 ⁒ ln ⁑ ( 2 ⁒ Ο€ ) + k = 2 ( 1 ) k ⁒ B k ⁑ ( h ) k ⁒ ( k 1 ) ⁒ z k 1 ,
28: 22.16 Related Functions
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22.16.1 am ⁑ ( x , k ) = Arcsin ⁑ ( sn ⁑ ( x , k ) ) , x ℝ ,
29: Errata
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  • Subsection 19.11(i)

    A sentence and unnumbered equation

    R C ⁑ ( Ξ³ Ξ΄ , Ξ³ ) = 1 Ξ΄ ⁒ arctan ⁑ ( Ξ΄ ⁒ sin ⁑ ΞΈ ⁒ sin ⁑ Ο• ⁒ sin ⁑ ψ Ξ± 2 1 Ξ± 2 ⁒ cos ⁑ ΞΈ ⁒ cos ⁑ Ο• ⁒ cos ⁑ ψ ) ,

    were added which indicate that care must be taken with the multivalued functions in (19.11.5). See (Cayley, 1961, pp. 103-106).

    Suggested by Albert Groenenboom.

  • β–Ί
  • Paragraph Confluent Hypergeometric Functions (in §7.18(iv))

    A note about the multivalued nature of the Kummer confluent hypergeometric function of the second kind U on the right-hand side of (7.18.10) was inserted.

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  • Equations (5.9.10), (5.9.11), (5.10.1), (5.11.1), (5.11.8)

    To increase the regions of validity the logarithms of the gamma function that appears on their left-hand sides have all been changed to Ln ⁑ Ξ“ ⁑ ( ) , where Ln is the general logarithm. Originally ln ⁑ Ξ“ ⁑ ( ) was used, where ln is the principal branch of the logarithm. These changes were recommended by Philippe Spindel on 2015-02-06.

  • 30: 10.18 Modulus and Phase Functions
    §10.18 Modulus and Phase Functions
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    §10.18(i) Definitions
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    §10.18(ii) Basic Properties
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    §10.18(iii) Asymptotic Expansions for Large Argument
    β–ΊIn (10.18.17) and (10.18.18) the remainder after n terms does not exceed the ( n + 1 ) th term in absolute value and is of the same sign, provided that n > Ξ½ 1 2 for (10.18.17) and 3 2 Ξ½ 3 2 for (10.18.18).