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Jacobi imaginary transformation

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21: 31.2 Differential Equations
Jacobi’s Elliptic Form
F -Homotopic Transformations
By composing these three steps, there result 2 3 = 8 possible transformations of the dependent variable (including the identity transformation) that preserve the form of (31.2.1).
Homographic Transformations
Composite Transformations
22: 18.33 Polynomials Orthogonal on the Unit Circle
Assume that w ( e i ϕ ) = w ( e i ϕ ) . …
w 1 ( x ) = ( 1 x 2 ) 1 2 w ( x + i ( 1 x 2 ) 1 2 ) ,
After a quadratic transformation (18.2.23) this would express OP’s on [ 1 , 1 ] with an even orthogonality measure in terms of the ϕ n . … Askey (1982a) and Sri Ranga (2010) give more general results leading to what seem to be the right analogues of Jacobi polynomials on the unit circle. …
18.33.19 d μ ( z ) = 1 2 π i w ( z ) d z z
23: Errata
  • Equation (23.6.11)
    23.6.11 σ ( ω 2 ) = 2 ω 1 exp ( 1 2 η 1 ( ω 1 τ 2 + ω 3 ω 2 ) ) θ 3 ( 0 , q ) π q 1 / 4 θ 1 ( 0 , q )

    The factor 2 ω 1 i exp ( 1 2 η 1 ω 1 τ 2 ) has been corrected to be 2 ω 1 exp ( 1 2 η 1 ( ω 1 τ 2 + ω 3 ω 2 ) ) .

  • Equation (23.6.12)
    23.6.12 σ ( ω 3 ) = 2 i ω 1 exp ( 1 2 η 1 ω 1 τ 2 ) θ 4 ( 0 , q ) π q 1 / 4 θ 1 ( 0 , q )

    The factor 2 ω 1 exp ( 1 2 η 1 ω 1 ) has been corrected to be 2 i ω 1 exp ( 1 2 η 1 ω 1 τ 2 ) .

  • Section 1.14

    There have been extensive changes in the notation used for the integral transforms defined in §1.14. These changes are applied throughout the DLMF. The following table summarizes the changes.

    Transform New Abbreviated Old
    Notation Notation Notation
    Fourier ( f ) ( x ) f ( x )
    Fourier Cosine c ( f ) ( x ) c f ( x )
    Fourier Sine s ( f ) ( x ) s f ( x )
    Laplace ( f ) ( s ) f ( s ) ( f ( t ) ; s )
    Mellin ( f ) ( s ) f ( s ) ( f ; s )
    Hilbert ( f ) ( s ) f ( s ) ( f ; s )
    Stieltjes 𝒮 ( f ) ( s ) 𝒮 f ( s ) 𝒮 ( f ; s )

    Previously, for the Fourier, Fourier cosine and Fourier sine transforms, either temporary local notations were used or the Fourier integrals were written out explicitly.

  • Table 22.4.3

    Originally a minus sign was missing in the entries for cd u and dc u in the second column (headed z + K + i K ). The correct entries are k 1 ns z and k sn z . Note: These entries appear online but not in the published print edition. More specifically, Table 22.4.3 in the published print edition is restricted to the three Jacobian elliptic functions sn , cn , dn , whereas Table 22.4.3 covers all 12 Jacobian elliptic functions.

    u
    z + K z + K + i K z + i K z + 2 K z + 2 K + 2 i K z + 2 i K
    cd u sn z k 1 ns z k 1 dc z cd z cd z cd z
    dc u ns z k sn z k cd z dc z dc z dc z

    Reported 2014-02-28 by Svante Janson.

  • Table 22.5.2

    The entry for sn z at z = 3 2 ( K + i K ) has been corrected. The correct entry is ( 1 + i ) ( ( 1 + k ) 1 / 2 i ( 1 k ) 1 / 2 ) / ( 2 k 1 / 2 ) . Originally the terms ( 1 + k ) 1 / 2 and ( 1 k ) 1 / 2 were given incorrectly as ( 1 + k ) 1 / 2 and ( 1 k ) 1 / 2 .

    Similarly, the entry for dn z at z = 3 2 ( K + i K ) has been corrected. The correct entry is ( 1 + i ) k 1 / 2 ( ( 1 + k ) 1 / 2 + i ( 1 k ) 1 / 2 ) / 2 . Originally the terms ( 1 + k ) 1 / 2 and ( 1 k ) 1 / 2 were given incorrectly as ( 1 + k ) 1 / 2 and ( 1 k ) 1 / 2

    Reported 2014-02-28 by Svante Janson.

  • 24: 15.12 Asymptotic Approximations
    See also Dunster (1999) where the asymptotics of Jacobi polynomials is described; compare (15.9.1). …
    15.12.9 ( z + 1 ) 3 λ / 2 ( 2 λ ) c 1 𝐅 ( a + λ , b + 2 λ c ; z ) = λ 1 / 3 ( e π i ( a c + λ + ( 1 / 3 ) ) Ai ( e 2 π i / 3 λ 2 / 3 β 2 ) + e π i ( c a λ ( 1 / 3 ) ) Ai ( e 2 π i / 3 λ 2 / 3 β 2 ) ) ( a 0 ( ζ ) + O ( λ 1 ) ) + λ 2 / 3 ( e π i ( a c + λ + ( 2 / 3 ) ) Ai ( e 2 π i / 3 λ 2 / 3 β 2 ) + e π i ( c a λ ( 2 / 3 ) ) Ai ( e 2 π i / 3 λ 2 / 3 β 2 ) ) ( a 1 ( ζ ) + O ( λ 1 ) ) ,
    By combination of the foregoing results of this subsection with the linear transformations of §15.8(i) and the connection formulas of §15.10(ii), similar asymptotic approximations for F ( a + e 1 λ , b + e 2 λ ; c + e 3 λ ; z ) can be obtained with e j = ± 1 or 0 , j = 1 , 2 , 3 . …