Logarithmic integral function

The logarithmic integral has an integral representation defined for all positive real numbers x ≠ 1 by the definite integral

${\displaystyle \operatorname {li} (x)=\int _{0}^{x}{\frac {dt}{\ln t}}.}$

Here, ln denotes the natural logarithm. The function 1/(ln t) has a singularity at t = 1, and the integral for x > 1 is interpreted as a Cauchy principal value,

${\displaystyle \operatorname {li} (x)=\lim _{\varepsilon \to 0+}\left(\int _{0}^{1-\varepsilon }{\frac {dt}{\ln t}}+\int _{1+\varepsilon }^{x}{\frac {dt}{\ln t}}\right).}$

The offset logarithmic integral or Eulerian logarithmic integral is defined as

${\displaystyle \operatorname {Li} (x)=\int _{2}^{x}{\frac {dt}{\ln t}}=\operatorname {li} (x)-\operatorname {li} (2).}$

As such, the integral representation has the advantage of avoiding the singularity in the domain of integration.

Equivalently,

${\displaystyle \operatorname {li} (x)=\int _{0}^{x}{\frac {dt}{\ln t}}=\operatorname {Li} (x)+\operatorname {li} (2).}$

The function li(x) has a single positive zero; it occurs at x ≈ 1.45136 92348 83381 05028 39684 85892 02744 94930... OEIS: A070769; this number is known as the Ramanujan–Soldner constant.

li(Li^-1(0)) = li(2) ≈ 1.045163 780117 492784 844588 889194 613136 522615 578151... OEIS: A069284

This is ${\displaystyle -(\Gamma \left(0,-\ln 2\right)+i\,\pi )}$ where ${\displaystyle \Gamma \left(a,x\right)}$ is the incomplete gamma function. It must be understood as the Cauchy principal value of the function.

The function li(x) is related to the exponential integral Ei(x) via the equation

${\displaystyle {\hbox{li}}(x)={\hbox{Ei}}(\ln x),\,\!}$

which is valid for x > 0. This identity provides a series representation of li(x) as

${\displaystyle \operatorname {li} (e^{u})={\hbox{Ei}}(u)=\gamma +\ln |u|+\sum _{n=1}^{\infty }{u^{n} \over n\cdot n!}\quad {\text{ for }}u\neq 0\;,}$

where γ ≈ 0.57721 56649 01532 ... OEIS: A001620 is the Euler–Mascheroni constant. A more rapidly convergent series by Ramanujan [1] is

${\displaystyle \operatorname {li} (x)=\gamma +\ln \ln x+{\sqrt {x}}\sum _{n=1}^{\infty }{\frac {(-1)^{n-1}(\ln x)^{n}}{n!\,2^{n-1}}}\sum _{k=0}^{\lfloor (n-1)/2\rfloor }{\frac {1}{2k+1}}.}$

The asymptotic behavior for x → ∞ is

${\displaystyle \operatorname {li} (x)=O\left({\frac {x}{\ln x}}\right).}$

where ${\displaystyle O}$ is the big O notation. The full asymptotic expansion is

${\displaystyle \operatorname {li} (x)\sim {\frac {x}{\ln x}}\sum _{k=0}^{\infty }{\frac {k!}{(\ln x)^{k}}}}$

or

${\displaystyle {\frac {\operatorname {li} (x)}{x/\ln x}}\sim 1+{\frac {1}{\ln x}}+{\frac {2}{(\ln x)^{2}}}+{\frac {6}{(\ln x)^{3}}}+\cdots .}$

This gives the following more accurate asymptotic behaviour:

${\displaystyle \operatorname {li} (x)-{\frac {x}{\ln x}}=O\left({\frac {x}{(\ln x)^{2}}}\right).}$

As an asymptotic expansion, this series is not convergent: it is a reasonable approximation only if the series is truncated at a finite number of terms, and only large values of x are employed. This expansion follows directly from the asymptotic expansion for the exponential integral.

This implies e.g. that we can bracket li as:

${\displaystyle 1+{\frac {1}{\ln x}}<\operatorname {li} (x){\frac {\ln x}{x}}<1+{\frac {1}{\ln x}}+{\frac {3}{(\ln x)^{2}}}}$

for all ${\displaystyle \ln x\geq 11}$.

The logarithmic integral is important in number theory, appearing in estimates of the number of prime numbers less than a given value. For example, the prime number theorem states that:

${\displaystyle \pi (x)\sim \operatorname {li} (x)}$

where ${\displaystyle \pi (x)}$ denotes the number of primes smaller than or equal to ${\displaystyle x}$.

Assuming the Riemann hypothesis, we get the even stronger:[2]

${\displaystyle |\operatorname {li} (x)-\pi (x)|=O({\sqrt {x}}\log x)}$

In fact, the Riemann hypothesis is equivalent to the statement that:

${\displaystyle |\operatorname {li} (x)-\pi (x)|=O(x^{1/2+a})}$ for any ${\displaystyle a>0}$.

For small ${\displaystyle x}$, ${\displaystyle \operatorname {li} (x)>\pi (x)}$ but the difference changes sign an infinite number of times as ${\displaystyle x}$ increases, and the first time this happens is somewhere between 10¹⁹ and 1.4×10³¹⁶.

• Jørgen Pedersen Gram
• Skewes' number
• List of integrals of logarithmic functions

• Abramowitz, Milton; Stegun, Irene Ann, eds. (1983) [June 1964]. "Chapter 5". Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables. Applied Mathematics Series. Vol. 55 (Ninth reprint with additional corrections of tenth original printing with corrections (December 1972); first ed.). Washington D.C.; New York: United States Department of Commerce, National Bureau of Standards; Dover Publications. p. 228. ISBN 978-0-486-61272-0. LCCN 64-60036. MR 0167642. LCCN 65-12253.
• Temme, N. M. (2010), "Exponential, Logarithmic, Sine, and Cosine Integrals", in Olver, Frank W. J.; Lozier, Daniel M.; Boisvert, Ronald F.; Clark, Charles W. (eds.), NIST Handbook of Mathematical Functions, Cambridge University Press, ISBN 978-0-521-19225-5, MR 2723248.