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relation to sine and cosine integrals

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11: 14.5 Special Values
§14.5(v) μ = 0 , ν = ± 1 2
In this subsection K ( k ) and E ( k ) denote the complete elliptic integrals of the first and second kinds; see §19.2(ii). …
§14.5(vi) Addendum to §14.5(ii) μ = 0 , ν = 2
12: 28.10 Integral Equations
§28.10 Integral Equations
§28.10(i) Equations with Elementary Kernels
§28.10(ii) Equations with Bessel-Function Kernels
§28.10(iii) Further Equations
For relations with variable boundaries see Volkmer (1983).
13: 19.6 Special Cases
14: Bibliography S
  • D. Schmidt and G. Wolf (1979) A method of generating integral relations by the simultaneous separability of generalized Schrödinger equations. SIAM J. Math. Anal. 10 (4), pp. 823–838.
  • D. V. Slavić (1974) Complements to asymptotic development of sine cosine integrals, and auxiliary functions. Univ. Beograd. Publ. Elecktrotehn. Fak., Ser. Mat. Fiz. 461–497, pp. 185–191.
  • B. D. Sleeman (1968a) Integral equations and relations for Lamé functions and ellipsoidal wave functions. Proc. Cambridge Philos. Soc. 64, pp. 113–126.
  • D. M. Smith (2011) Algorithm 911: multiple-precision exponential integral and related functions. ACM Trans. Math. Software 37 (4), pp. Art. 46, 16.
  • I. A. Stegun and R. Zucker (1976) Automatic computing methods for special functions. III. The sine, cosine, exponential integrals, and related functions. J. Res. Nat. Bur. Standards Sect. B 80B (2), pp. 291–311.
  • 15: Bibliography M
  • A. J. MacLeod (1996b) Rational approximations, software and test methods for sine and cosine integrals. Numer. Algorithms 12 (3-4), pp. 259–272.
  • I. Marquette and C. Quesne (2016) Connection between quantum systems involving the fourth Painlevé transcendent and k -step rational extensions of the harmonic oscillator related to Hermite exceptional orthogonal polynomial. J. Math. Phys. 57 (5), pp. Paper 052101, 15 pp..
  • M. Micu (1968) Recursion relations for the 3 - j symbols. Nuclear Physics A 113 (1), pp. 215–220.
  • G. J. Miel (1981) Evaluation of complex logarithms and related functions. SIAM J. Numer. Anal. 18 (4), pp. 744–750.
  • S. C. Milne (1985c) A new symmetry related to 𝑆𝑈 ( n ) for classical basic hypergeometric series. Adv. in Math. 57 (1), pp. 71–90.
  • 16: 1.17 Integral and Series Representations of the Dirac Delta
    §1.17 Integral and Series Representations of the Dirac Delta
    §1.17(ii) Integral Representations
    The inner integral does not converge. …
    Sine and Cosine Functions
    Equations (1.17.12_1) through (1.17.16) may re-interpreted as spectral representations of completeness relations, expressed in terms of Dirac delta distributions, as discussed in §1.18(v), and §1.18(vi) Further mathematical underpinnings are referenced in §1.17(iv). …
    17: 10.9 Integral Representations
    Poisson’s and Related Integrals
    Schläfli’s and Related Integrals
    Mehler–Sonine and Related Integrals
    §10.9(ii) Contour Integrals
    See Paris and Kaminski (2001, p. 116) for related results. …
    18: 19.10 Relations to Other Functions
    §19.10 Relations to Other Functions
    §19.10(i) Theta and Elliptic Functions
    For relations of Legendre’s integrals to theta functions, Jacobian functions, and Weierstrass functions, see §§20.9(i), 22.15(ii), and 23.6(iv), respectively. …
    §19.10(ii) Elementary Functions
    In each case when y = 1 , the quantity multiplying R C supplies the asymptotic behavior of the left-hand side as the left-hand side tends to 0. …
    19: 19.7 Connection Formulas
    Legendre’s Relation
    §19.7(iii) Change of Parameter of Π ( ϕ , α 2 , k )
    There are three relations connecting Π ( ϕ , α 2 , k ) and Π ( ϕ , ω 2 , k ) , where ω 2 is a rational function of α 2 . … The first of the three relations maps each circular region onto itself and each hyperbolic region onto the other; in particular, it gives the Cauchy principal value of Π ( ϕ , α 2 , k ) when α 2 > csc 2 ϕ (see (19.6.5) for the complete case). … The third relation (missing from the literature of Legendre’s integrals) maps each circular region onto the other and each hyperbolic region onto the other: …
    20: 22.11 Fourier and Hyperbolic Series
    22.11.3 dn ( z , k ) = π 2 K + 2 π K n = 1 q n cos ( 2 n ζ ) 1 + q 2 n .
    Next, with E = E ( k ) denoting the complete elliptic integral of the second kind (§19.2(ii)) and q exp ( 2 | ζ | ) < 1 ,
    22.11.13 sn 2 ( z , k ) = 1 k 2 ( 1 E K ) 2 π 2 k 2 K 2 n = 1 n q n 1 q 2 n cos ( 2 n ζ ) .
    A related hyperbolic series is …where E = E ( k ) is defined by §19.2.9. …