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21: 7.21 Physical Applications
§7.21 Physical Applications
The error functions, Fresnel integrals, and related functions occur in a variety of physical applications. … Carslaw and Jaeger (1959) gives many applications and points out the importance of the repeated integrals of the complementary error function i n erfc ( z ) . …Efficient algorithms for computing the Faddeeva (or Faddeyeva) function are discussed in Wells (1999), a paper frequently cited in the astrophysics literature. … Dawson’s integral appears in de-convolving even more complex motional effects; see Pratt (2007). …
22: 2.11 Remainder Terms; Stokes Phenomenon
As an example consider … From §8.19(i) the generalized exponential integral is given by … Two different asymptotic expansions in terms of elementary functions, (2.11.6) and (2.11.7), are available for the generalized exponential integral in the sector 1 2 π < ph z < 3 2 π . … Often the process of re-expansion can be repeated any number of times. … For example, using double precision d 20 is found to agree with (2.11.31) to 13D. …
23: Peter L. Walker
Walker’s books are An Introduction to Complex Analysis, published by Hilger in 1974, The Theory of Fourier Series and Integrals, published by Wiley in 1986, Elliptic Functions. A Constructive Approach, published by Wiley in 1996, and Examples and Theorems in Analysis, published by Springer in 2004. …
  • 24: 7.8 Inequalities
    §7.8 Inequalities
    7.8.5 x 2 2 x 2 + 1 x 2 ( 2 x 2 + 5 ) 4 x 4 + 12 x 2 + 3 x 𝖬 ( x ) < 2 x 4 + 9 x 2 + 4 4 x 4 + 20 x 2 + 15 < x 2 + 1 2 x 2 + 3 , x 0 .
    7.8.7 sinh x 2 x < e x 2 F ( x ) = 0 x e t 2 d t < e x 2 1 x , x > 0 .
    The function F ( x ) / 1 e 2 x 2 is strictly decreasing for x > 0 . For these and similar results for Dawson’s integral F ( x ) see Janssen (2021). …
    25: Bibliography
  • M. J. Ablowitz and H. Segur (1977) Exact linearization of a Painlevé transcendent. Phys. Rev. Lett. 38 (20), pp. 1103–1106.
  • A. Adelberg (1992) On the degrees of irreducible factors of higher order Bernoulli polynomials. Acta Arith. 62 (4), pp. 329–342.
  • S. V. Aksenov, M. A. Savageau, U. D. Jentschura, J. Becher, G. Soff, and P. J. Mohr (2003) Application of the combined nonlinear-condensation transformation to problems in statistical analysis and theoretical physics. Comput. Phys. Comm. 150 (1), pp. 1–20.
  • Z. Altaç (1996) Integrals involving Bickley and Bessel functions in radiative transfer, and generalized exponential integral functions. J. Heat Transfer 118 (3), pp. 789–792.
  • D. E. Amos (1989) Repeated integrals and derivatives of K Bessel functions. SIAM J. Math. Anal. 20 (1), pp. 169–175.
  • 26: 10.75 Tables
  • Achenbach (1986) tabulates J 0 ( x ) , J 1 ( x ) , Y 0 ( x ) , Y 1 ( x ) , x = 0 ( .1 ) 8 , 20D or 18–20S.

  • Zhang and Jin (1996, p. 270) tabulates 0 x J 0 ( t ) d t , 0 x t 1 ( 1 J 0 ( t ) ) d t , 0 x Y 0 ( t ) d t , x t 1 Y 0 ( t ) d t , x = 0 ( .1 ) 1 ( .5 ) 20 , 8D.

  • Bickley et al. (1952) tabulates x n I n ( x ) or e x I n ( x ) , x n K n ( x ) or e x K n ( x ) , n = 2 ( 1 ) 20 , x = 0 (.01 or .1) 10(.1) 20, 8S; I n ( x ) , K n ( x ) , n = 0 ( 1 ) 20 , x = 0 or 0.1 ( .1 ) 20 , 10S.

  • Kerimov and Skorokhodov (1984b) tabulates all zeros of the principal values of K n ( z ) and K n ( z ) , for n = 2 ( 1 ) 20 , 9S.

  • Zhang and Jin (1996, p. 271) tabulates e x 0 x I 0 ( t ) d t , e x 0 x t 1 ( I 0 ( t ) 1 ) d t , e x x K 0 ( t ) d t , x e x x t 1 K 0 ( t ) d t , x = 0 ( .1 ) 1 ( .5 ) 20 , 8D.

  • 27: 22.3 Graphics
    §22.3(i) Real Variables: Line Graphs
    §22.3(iii) Complex z ; Real k
    In the graphics shown in this subsection height corresponds to the absolute value of the function and color to the phase. …
    §22.3(iv) Complex k
    In Figures 22.3.24 and 22.3.25, height corresponds to the absolute value of the function and color to the phase. …
    28: 7.25 Software
    §7.25(ii) erf x , erfc x , i n erfc ( x ) , x
    §7.25(iv) C ( x ) , S ( x ) , f ( x ) , g ( x ) , x
    §7.25(v) C ( z ) , S ( z ) , z
    §7.25(vi) ( x ) , G ( x ) , 𝖴 ( x , t ) , 𝖵 ( x , t ) , x
    §7.25(vii) ( z ) , G ( z ) , z
    29: 19.36 Methods of Computation
    Numerical differences between the variables of a symmetric integral can be reduced in magnitude by successive factors of 4 by repeated applications of the duplication theorem, as shown by (19.26.18). … Lee (1990) compares the use of theta functions for computation of K ( k ) , E ( k ) , and K ( k ) E ( k ) , 0 k 2 1 , with four other methods. …For computation of Legendre’s integral of the third kind, see Abramowitz and Stegun (1964, §§17.7 and 17.8, Examples 15, 17, 19, and 20). … Similarly, §19.26(ii) eases the computation of functions such as R F ( x , y , z ) when x ( > 0 ) is small compared with min ( y , z ) . …
    30: 8 Incomplete Gamma and Related
    Functions
    Chapter 8 Incomplete Gamma and Related Functions