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6 Exponential, Logarithmic, Sine, and Cosine IntegralsProperties

§6.10 Other Series Expansions

Contents
  1. §6.10(i) Inverse Factorial Series
  2. §6.10(ii) Expansions in Series of Spherical Bessel Functions

§6.10(i) Inverse Factorial Series

6.10.1 E1⁡(z)=e−z⁢(c0z+c1z⁢(z+1)+2!⁢c2z⁢(z+1)⁢(z+2)+3!⁢c3z⁢(z+1)⁢(z+2)⁢(z+3)+⋯),
ℜ⁡z>0,

where

6.10.2 c0 =1,
c1 =−1,
c2 =12,
c3 =−13,
c4 =16,

and

6.10.3 ck=−∑j=0k−1cjk−j,
k≥1.

For a more general result (incomplete gamma function), and also for a result for the logarithmic integral, see Nielsen (1906a, p. 283: Formula (3) is incorrect).

§6.10(ii) Expansions in Series of Spherical Bessel Functions

For the notation see §10.47(ii).

6.10.4 Si⁡(z) =z⁢∑n=0∞(𝗃n⁡(12⁢z))2,
6.10.5 Cin⁡(z) =∑n=1∞an⁢(𝗃n⁡(12⁢z))2,
6.10.6 Ei⁡(x)=γ+ln⁡|x|+∑n=0∞(−1)n⁢(x−an)⁢(𝗂n(1)⁡(12⁢x))2,
x≠0,

where

6.10.7 an=(2⁢n+1)⁢(1−(−1)n+ψ⁡(n+1)−ψ⁡(1)),

and ψ denotes the logarithmic derivative of the gamma function (§5.2(i)).

6.10.8 Ein⁡(z)=z⁢e−z/2⁢(𝗂0(1)⁡(12⁢z)+∑n=1∞2⁢n+1n⁢(n+1)⁢𝗂n(1)⁡(12⁢z)).

For (6.10.4)–(6.10.8) and further results see Harris (2000) and Luke (1969b, pp. 56–57). An expansion for E1⁡(z) can be obtained by combining (6.2.4) and (6.10.8).