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11: Guide to Searching the DLMF
Table 2: Wildcard Examples
Query What it stands for
si$ si, sin, sine, sinh, sinc, sinInt, similar, …
DLMF search is generally case-insensitive except when it is important to be case-sensitive, as when two different special functions have the same standard names but one name has a lower-case initial and the other is has an upper-case initial, such as si and Si, gamma and Gamma. …
  • The following standard special functions: si, Si, ci, Ci, shi, Shi, ce, Ce, se, Se, ln, Ln, Lommels, LommelS, Jacobiphi, and the list is still growing.

  • 12: 6.5 Further Interrelations
    6.5.3 1 2 ( Ei ( x ) + E 1 ( x ) ) = Shi ( x ) = i Si ( i x ) ,
    6.5.5 Si ( z ) = 1 2 i ( E 1 ( i z ) E 1 ( i z ) ) + 1 2 π ,
    13: 6.20 Approximations
  • Luke and Wimp (1963) covers Ei ( x ) for x 4 (20D), and Si ( x ) and Ci ( x ) for x 4 (20D).

  • Luke (1969b, pp. 41–42) gives Chebyshev expansions of Ein ( a x ) , Si ( a x ) , and Cin ( a x ) for 1 x 1 , a . The coefficients are given in terms of series of Bessel functions.

  • Luke (1969b, pp. 402, 410, and 415–421) gives main diagonal Padé approximations for Ein ( z ) , Si ( z ) , Cin ( z ) (valid near the origin), and E 1 ( z ) (valid for large | z | ); approximate errors are given for a selection of z -values.

  • 14: 10.15 Derivatives with Respect to Order
    For the notations Ci and Si see §6.2(ii). …
    10.15.9 Y ν ( x ) ν | ν = 1 2 = 2 π x ( Ci ( 2 x ) sin x ( Si ( 2 x ) π ) cos x ) .
    15: 6.6 Power Series
    6.6.5 Si ( z ) = n = 0 ( 1 ) n z 2 n + 1 ( 2 n + 1 ) ! ( 2 n + 1 ) ,
    16: 6.16 Mathematical Applications
    6.16.2 S n ( x ) = k = 0 n 1 sin ( ( 2 k + 1 ) x ) 2 k + 1 = 1 2 0 x sin ( 2 n t ) sin t d t = 1 2 Si ( 2 n x ) + R n ( x ) ,
    The first maximum of 1 2 Si ( x ) for positive x occurs at x = π and equals ( 1.1789 ) × 1 4 π ; compare Figure 6.3.2. …
    17: 6.10 Other Series Expansions
    6.10.4 Si ( z ) = z n = 0 ( 𝗃 n ( 1 2 z ) ) 2 ,
    18: 6.18 Methods of Computation
    Zeros of Ci ( x ) and si ( x ) can be computed to high precision by Newton’s rule (§3.8(ii)), using values supplied by the asymptotic expansion (6.13.2) as initial approximations. …
    19: 10.60 Sums
    10.60.11 n = 0 𝗃 n 2 ( z ) = Si ( 2 z ) 2 z .
    For Si see §6.2(ii). …
    20: 6.7 Integral Representations
    6.7.9 si ( z ) = 0 π / 2 e z cos t cos ( z sin t ) d t ,